master
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a Code for the Combination of Indirect and Direct Constraints on High Energy Physics Models |
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master
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a Code for the Combination of Indirect and Direct Constraints on High Energy Physics Models |
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A model class for new physics in the form of the dimension-six effective Lagrangian. More...
#include <NPSMEFTd6.h>
Inheritance diagram for NPSMEFTd6:A model class for new physics in the form of the dimension-six effective Lagrangian.
This is a Model class containing parameters and functions associated with the general dimension-six effective Lagrangian. (Use the model name "NPSMEFTd6_LFU_QFU" to assume lepton and quark flavour universality)
In this class we consider the dimension-six effective Lagrangian
\[ \mathcal{L}_\mathrm{eff} = \mathcal{L}_\mathrm{SM} + \sum_i \frac{C_i}{\Lambda^2} \mathcal{O}_i. \]
The implementation is written in the basis of [132]. For convenience, the parameterization also includes operators appearing in other common bases. In particular, the complete set of parameters contains 4 redundancies, given by the coefficients \(C_{2B,2W,DHB,DHW,DB,DW} \), which correspond to operators not included in the basis of [132]. For meaningful physical results one must make sure to include only a complete set of interactions in a given analysis.
After creating an instance of the current class with the constructor NPSMEFTd6(), it is required to call the initialization method InitializeModel(). In the Monte Carlo run, the constructor as well as the initialization method are called in InputParser::ReadParameters().
The model parameters of NPSMEFTd6 are summarized below:
| Label | LaTeX symbol | Description |
|---|---|---|
| CG | \(C_{G} \) | The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\). |
| CW | \(C_{W} \) | The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\). |
| C2B | \(C_{2B} \) | The coefficient of the operator \({\cal O}_{2B}=\frac 12 (\partial_\rho B_{\mu\nu})^2\). (Implemented via EOM.) |
| C2W | \(C_{2W} \) | The coefficient of the operator \({\cal O}_{2W}=\frac 12 (D_\rho W_{\mu\nu}^{a})^2\). (Implemented via EOM.) |
| C2BS | \(C_{2B}^{SILH} \) | The coefficient of the SILH operator \({\cal O}_{2B}^{SILH}=\frac 12 (\partial^\mu B_{\mu\nu})(\partial_\rho B^{\rho\nu})\). (Implemented via EOM.) |
| C2WS | \(C_{2W}^{SILH} \) | The coefficient of the operator \({\cal O}_{2W}^{SILH}=\frac 12 (D_\mu W^{a~\!\mu\nu})(D^\rho W_{\rho\nu}^{a})\). (Implemented via EOM.) |
| CHG | \(C_{HG} \) | The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\). |
| CHW | \(C_{HW} \) | The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\). |
| CHB | \(C_{HB} \) | The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\). |
| CDHB | \(C_{DHB} \) | The coefficient of the operator \({\cal O}_{DHB}=i\big(D^\mu H^\dagger D^\nu H\big) B_{\mu\nu}\). |
| CDHW | \(C_{DHW}\) | The coefficient of the operator \({\cal O}_{DHW}=i\big(D^\mu H^\dagger \sigma^a D^\nu H\big) W_{\mu\nu}^a\). |
| CDB | \(C_{DB} \) | The coefficient of the operator \({\cal O}_{DB}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^\mu H\big) \partial^\nu B_{\mu\nu}\). (Implemented via EOM.) |
| CDW | \(C_{DW}\) | The coefficient of the operator \({\cal O}_{DW}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^{a~\!\mu} H\big) D^\nu W_{\mu\nu}^a\). (Implemented via EOM.) |
| CWB | \(C_{WB} \) | The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\sigma^a H\big)W_{\mu\nu}^a B^{\mu\nu}\). |
| CHD | \(C_{HD}\) | The coefficient of the operator \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\). |
| CT | \(C_{T}\) | The coefficient of the operator \({\cal O}_{T}=\frac{1}{2} \big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big)^2\). |
| CHbox | \(C_{H\Box}\) | The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\). |
| CH | \(C_{H}\) | The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\). |
| CHL1_kk, CHL1_klr, CHL1_kli | \( (C_{HL}^{(1)})_{kk}, \mbox{Re}\big[(C_{HL}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(1)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^j\big)\), for \(i,j=1,2,3\). |
| CHL3_kk, CHL3_klr, CHL3_kli | \( (C_{HL}^{(3)})_{kk}, \mbox{Re}\big[(C_{HL}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(3)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \sigma^a L^j\big)\), for \(i,j=1,2,3\). |
| CHe_kk, CHe_klr, CHe_kli | \( (C_{He})_{kk}, \mbox{Re}\big[(C_{He})_{kl}\big], \mbox{Im}\big[(C_{He})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^j\big)\), for \(i,j=1,2,3\). |
| CHQ1_kk, CHQ1_klr, CHQ1_kli | \( (C_{HQ}^{(1)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(1)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^j\big)\), for \(i,j=1,2,3\). |
| CHQ3_kk, CHQ3_klr, CHQ3_kli | \( (C_{HQ}^{(3)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(3)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \sigma^a Q^j\big)\), for \(i,j=1,2,3\). |
| CHu_kk, CHu_klr, CHu_kli | \( (C_{Hu})_{kk}, \mbox{Re}\big[(C_{Hu})_{kl}\big], \mbox{Im}\big[(C_{Hu})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hu})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^j\big)\), for \(i,j=1,2,3\). |
| CHd_kk, CHd_klr, CHd_kli | \( (C_{Hd})_{kk}, \mbox{Re}\big[(C_{Hd})_{kl}\big], \mbox{Im}\big[(C_{Hd})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hd})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\). |
| CHud_klr, CHud_kli | \(\mbox{Re}\big[(C_{Hud})_{kl}\big], \mbox{Im}\big[(C_{Hud})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ij} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\). |
| CeH_klr, CeH_kli | \(\mbox{Re}\big[(C_{eH})_{kl}\big], \mbox{Im}\big[(C_{eH})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{ij} =\big(H^\dagger H\big) \big(\overline{L^i}\,H E^j\big)\), for \(i,j=1,2,3\). |
| CuH_klr, CuH_kli | \(\mbox{Re}\big[(C_{uH})_{kl}\big], \mbox{Im}\big[(C_{uH})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,\widetilde{H} U^j\big)\), for \(i,j=1,2,3\). |
| CdH_klr, CdH_kli | \(\mbox{Re}\big[(C_{dH})_{kl}\big], \mbox{Im}\big[(C_{dH})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,H D^j\big)\), for \(i,j=1,2,3\). |
| CuG_klr, CuG_kli | \(\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\), for \(i,j=1,2,3\). |
| CuW_klr, CuW_kli | \(\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a U^j\big)\widetilde{H} W_{\mu\nu}^a\), for \(i,j=1,2,3\). |
| CuB_klr, CuB_kli | \(\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\), for \(i,j=1,2,3\). |
| CdG_klr, CdG_kli | \(\mbox{Re}\big[(C_{dG})_{kl}\big], \mbox{Im}\big[(C_{dG})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A D^j\big)H G_{\mu\nu}^A\), for \(i,j=1,2,3\). |
| CdW_klr, CdW_kli | \(\mbox{Re}\big[(C_{dW})_{kl}\big], \mbox{Im}\big[(C_{dW})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a D^j\big)H W_{\mu\nu}^a\), for \(i,j=1,2,3\). |
| CdB_klr, CdB_kli | \(\mbox{Re}\big[(C_{dB})_{kl}\big], \mbox{Im}\big[(C_{dB})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} D^j\big)H B_{\mu\nu}\), for \(i,j=1,2,3\). |
| CeW_klr, CeW_kli | \(\mbox{Re}\big[(C_{eW})_{kl}\big], \mbox{Im}\big[(C_{eW})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eW})_{ij} =\big(\overline{L^i}\sigma^{\mu\nu} \sigma_a E^j\big)H W_{\mu\nu}^a\), for \(i,j=1,2,3\). |
| CeB_klr, CeB_kli | \(\mbox{Re}\big[(C_{eB})_{kl}\big], \mbox{Im}\big[(C_{eB})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eB})_{ij} =\big(\overline{L^i}\sigma^{\mu\nu} E^j\big)H B_{\mu\nu}\), for \(i,j=1,2,3\). |
| CLL_1221, CLL_2112 | \((C_{LL})_{1221,2112}\) | The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\). |
| CLQ1 | \(C_{LQ}^{(1)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\). |
| CLQ3 | \(C_{LQ}^{(3)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \sigma_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)\). |
| Cee | \(C_{EE}\) | The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Ceu | \(C_{EU}\) | The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| Ced | \(C_{ED}\) | The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CLe | \(C_{LE}\) | The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| CLu | \(C_{LU}\) | The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| CLd | \(C_{LD}\) | The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CQe | \(C_{QE}\) | The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Lambda_NP | \(\Lambda \) | The new physics scale. |
| BrHinv | Br \((H\to invisible)\) | The branching ratio of invisible Higgs decays. Only the absolute value of this parameter is considered.(Not part of the EFT. Only for tests.) |
| BrHexo | Br \((H\to exotic)\) | The branching ratio of exotic Higgs decays. Only the absolute value of this parameter is considered. (Not part of the EFT. Only for tests.) |
| dg1Z | \(\delta g_{1Z}\) | Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.) |
| dKappaga | \(\delta \kappa_{\gamma}\) | Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.) |
| lambZ | \(\lambda_{Z}\) | Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.) |
| eXint | \(\varepsilon_{X}^{int}\) | The relative intrinsic theoretical uncertainty for the process X. (Only for Higgs observables and assumed to be constant in the energy.) |
| eXpar | \(\varepsilon_{X}^{par}\) | The relative parametric theoretical uncertainty for the process X. (Only for Higgs observables and assumed to be constant in the energy.) |
| eVBFE_i | \(\varepsilon_{VBF}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the VBF production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HAA}, g_{HWW}^{(1,2,3)}, g_{Hgg}, g_{HZuu,HZdd}^{L,R}, g_{HWud}^{L}, g_{Zuu,Zdd}^{L,R}, g_{Wud}^{L})\) |
| eWHE_i | \(\varepsilon_{WH}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the WH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{HWW}^{(1,2,3)}, g_{HWud}^{L}, g_{Wud}^{L})\) |
| eZHE_i | \(\varepsilon_{ZH}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ZH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HZuu,HZdd}^{L,R}, g_{Zuu,Zdd}^{L,R})\) |
| ettHE_i | \(\varepsilon_{ttH}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ttH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{Htt}, g_{Hgg})\) |
Where the hermitian derivatives are defined as
\[ H^\dagger i \overset{\leftrightarrow}{D}_\mu H\equiv H^\dagger i(D_\mu - \overset{\leftarrow}{D}_\mu)H \]
and
\[ H^\dagger i \overset{\leftrightarrow}{D^a_\mu} H\equiv H^\dagger i (\sigma^a D_\mu - \overset{\leftarrow}{D}_\mu \sigma^a)H. \]
Alternatively, when using the model name "NPSMEFTd6_LFU_QFU", where lepton and quark flavour universality are assumed (except for \((C_{fH})_{ij},~f=e,u,d\) which are assumed to be diagonal only), the parameters to be used as inputs for the dimension six coefficients are the following:
| Label | LaTeX symbol | Description |
|---|---|---|
| CG | \(C_{G} \) | The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\). |
| CW | \(C_{W} \) | The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\). |
| C2B | \(C_{2B} \) | The coefficient of the operator \({\cal O}_{2B}=\frac 12 (\partial_\rho B_{\mu\nu})^2\). (Implemented via EOM.) |
| C2W | \(C_{2W} \) | The coefficient of the operator \({\cal O}_{2W}=\frac 12 (D_\rho W_{\mu\nu}^{a})^2\). (Implemented via EOM.) |
| C2BS | \(C_{2B}^{SILH} \) | The coefficient of the SILH operator \({\cal O}_{2B}^{SILH}=\frac 12 (\partial^\mu B_{\mu\nu})(\partial_\rho B^{\rho\nu})\). (Implemented via EOM.) |
| C2WS | \(C_{2W}^{SILH} \) | The coefficient of the operator \({\cal O}_{2W}^{SILH}=\frac 12 (D_\mu W^{a~\!\mu\nu})(D^\rho W_{\rho\nu}^{a})\). (Implemented via EOM.) |
| CHG | \(C_{HG} \) | The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\). |
| CHW | \(C_{HW} \) | The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\). |
| CHB | \(C_{HB} \) | The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\). |
| CDHB | \(C_{DHB} \) | The coefficient of the operator \({\cal O}_{DHB}=i\big(D^\mu H^\dagger D^\nu H\big) B_{\mu\nu}\). |
| CDHW | \(C_{DHW}\) | The coefficient of the operator \({\cal O}_{DHW}=i\big(D^\mu H^\dagger \sigma^a D^\nu H\big) W_{\mu\nu}^a\). |
| CDB | \(C_{DB} \) | The coefficient of the operator \({\cal O}_{DB}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^\mu H\big) \partial^\nu B_{\mu\nu}\). (Implemented via EOM.) |
| CDW | \(C_{DW}\) | The coefficient of the operator \({\cal O}_{DW}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^{a~\!\mu} H\big) D^\nu W_{\mu\nu}^a\). (Implemented via EOM.) |
| CWB | \(C_{WB} \) | The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\sigma^a H\big)W_{\mu\nu}^a B^{\mu\nu}\). |
| CHD | \(C_{HD}\) | The coefficient of the operator \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\). |
| CT | \(C_{T}\) | The coefficient of the operator \({\cal O}_{T}=\frac{1}{2} \big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big)^2\). |
| CHbox | \(C_{H\Box}\) | The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\). |
| CH | \(C_{H}\) | The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\). |
| CHL1 | \( (C_{HL}^{(1)})_{ii} \) | The coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^i\big)\) (flavor universal). |
| CHL3 | \( (C_{HL}^{(3)})_{ii} \) | The coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \sigma^a L^i\big)\) (flavor universal). |
| CHe | \( (C_{He})_{ii} \) | The coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^i\big)\) (flavor universal). |
| CHQ1 | \( (C_{HQ}^{(1)})_{ii} \) | The coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^i\big)\) (flavor universal). |
| CHQ3 | \( (C_{HQ}^{(3)})_{ii}\) | The coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \sigma^a Q^i\big)\) (flavor universal). |
| CHu | \( (C_{Hu})_{ii} \) | The coefficient of the operator \(({\cal O}_{Hu})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^i\big)\) (flavor universal). |
| CHd | \( (C_{Hd})_{ii} \) | The coefficient of the operator \(({\cal O}_{Hd})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^i\big)\) (flavor universal). |
| CHud_r, CHud_i | \(\mbox{Re}\big[(C_{Hud})_{ii}\big], \mbox{Im}\big[(C_{Hud})_{ii}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ii} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^i\big)\) (flavor universal). |
| CeH_jjr, CeH_jji | \(\mbox{Re}\big[(C_{eH})_{jj}\big], \mbox{Im}\big[(C_{eH})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{jj} =\big(H^\dagger H\big) \big(\overline{L^j}\,H E^j\big)\) (flavor universal). |
| CuH_jjr, CuH_jji | \(\mbox{Re}\big[(C_{uH})_{jj}\big], \mbox{Im}\big[(C_{uH})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{jj} =\big(H^\dagger H\big) \big(\overline{Q^j}\,\widetilde{H} U^j\big)\) (flavor universal). |
| CdH_jjr, CdH_jji | \(\mbox{Re}\big[(C_{dH})_{jj}\big], \mbox{Im}\big[(C_{dH})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{jj} =\big(H^\dagger H\big) \big(\overline{Q^j}\,H D^j\big)\) (flavor universal). |
| CuG_jjr, CuG_jji | \(\mbox{Re}\big[(C_{uG})_{jj}\big], \mbox{Im}\big[(C_{uG})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\) (flavor universal). |
| CuW_jjr, CuW_jji | \(\mbox{Re}\big[(C_{uW})_{jj}\big], \mbox{Im}\big[(C_{uW})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} \sigma_a U^j\big)\widetilde{H} W_{\mu\nu}^a\) (flavor universal). |
| CuB_jjr, CuB_jji | \(\mbox{Re}\big[(C_{uB})_{jj}\big], \mbox{Im}\big[(C_{uB})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\) (flavor universal). |
| CdG_jjr, CdG_jji | \(\mbox{Re}\big[(C_{dG})_{jj}\big], \mbox{Im}\big[(C_{dG})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dG})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} T_A D^j\big)H G_{\mu\nu}^A\) (flavor universal). |
| CdW_jjr, CdW_jji | \(\mbox{Re}\big[(C_{dW})_{jj}\big], \mbox{Im}\big[(C_{dW})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dW})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} \sigma_a D^j\big)H W_{\mu\nu}^a\) (flavor universal). |
| CdB_jjr, CdB_jji | \(\mbox{Re}\big[(C_{dB})_{jj}\big], \mbox{Im}\big[(C_{dB})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dB})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} D^j\big)H B_{\mu\nu}\) (flavor universal). |
| CeW_jjr, CeW_jji | \(\mbox{Re}\big[(C_{eW})_{jj}\big], \mbox{Im}\big[(C_{eW})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eW})_{jj} =\big(\overline{L^j}\sigma^{\mu\nu} \sigma_a E^j\big)H W_{\mu\nu}^a\) (flavor universal). |
| CeB_jjr, CeB_jji | \(\mbox{Re}\big[(C_{eB})_{jj}\big], \mbox{Im}\big[(C_{eB})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eB})_{jj} =\big(\overline{L^j}\sigma^{\mu\nu} E^j\big)H B_{\mu\nu}\) (flavor universal). |
| CLL | \((C_{LL})_{1221,2112}\) | The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\). |
| CLQ1 | \(C_{LQ}^{(1)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\). |
| CLQ3 | \(C_{LQ}^{(3)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \sigma_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)\). |
| Cee | \(C_{EE}\) | The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Ceu | \(C_{EU}\) | The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| Ced | \(C_{ED}\) | The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CLe | \(C_{LE}\) | The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| CLu | \(C_{LU}\) | The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| CLd | \(C_{LD}\) | The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CQe | \(C_{QE}\) | The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Lambda_NP | \(\Lambda \) | The new physics scale. |
| BrHinv | Br \((H\to invisible)\) | The branching ratio of invisible Higgs decays. (Not part of the EFT. Only for tests.) |
| BrHexo | Br \((H\to exotic)\) | The branching ratio of exotic Higgs decays. (Not part of the EFT. Only for tests.) |
(The parameters associated to the theoretical uncertainties: \(\varepsilon_{X}^{int}\), \(\varepsilon_{X}^{par}\) and \(\varepsilon_{X}^i(E)\), are the same for both "NPSMEFTd6" and "NPSMEFTd6_LFU_QFU".)
The Flags of NPSMEFTd6 are summarized below:
| Label | Value | Description |
|---|---|---|
| QuadraticTerms | TRUE / FALSE | This flag is set to TRUE if the quadratic terms in Higgs cross sections and widths are switched on. The default value is FALSE; new physics contributions are linearized. |
| RotateCHWCHB | TRUE / FALSE | This flag is set to TRUE if using {sW2*CHW+cW2*CHB, -cW2*CHW+sW2*CHB} instead of {CHW, CHB} as floating parameters. The default value is FALSE. |
| PartialQFU | TRUE / FALSE | This flag is set to TRUE if using CHQ1_11=CHQ1_22, CHQ3_11=CHQ3_22, CHU_11=CHU_22, CHD_11=CHD_22, CHud_11=CHud_22.} Only applies in the Non QFU case. In that case only the (1,1) component is taken into account. The default value is FALSE. |
| FlavU3OfX | TRUE / FALSE | This flag is set to TRUE if using \(U(3)^5\) flavour symmetry relations in the coefficients of the operators \(O_{fH}\) and \(O_{fV}\). If TRUE, the operator coefficient is proportional to the corresponding Yukawa matrix (diagonal), with the proportionality coefficient given by the Model parameter corresponding to the coefficient of third family. (Implemented only for the real and diagonal elements of the \(O_{fH}\) and \(O_{fV}\) operators.) The default value is FALSE. |
| FlagUnivOfX | TRUE / FALSE | This flag is set to TRUE if using \(U(3)^5\) flavour symmetry relations in the coefficients of the operators \(O_{fH}\) and \(O_{fV}\) plus they are the same for all fermions. If TRUE, all the operator coefficients are proportional to the corresponding Yukawa matrix (diagonal), with the proportionality coefficient given by the Model parameter corresponding to the coefficients of third family for \(O_{uH}\) and \(O_{uV}\), respectively. (Implemented only for the real and diagonal elements of the \(O_{fH}\) and \(O_{fV}\) operators.) The default value is FALSE. |
| HiggsSM | TRUE / FALSE | This flag is set to TRUE if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables. The default value is FALSE. |
| LoopHd6 | TRUE / FALSE | This flag is set to TRUE if including modifications in the SM loops in Higgs observables due to the dim 6 interactions. The default value is FALSE. |
| LoopH3d6Quad | TRUE / FALSE | This flag is set to TRUE if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling. Works independently of the flag QuadraticTerms (the quadratic contributions are also added if the latter is true). The default value is FALSE. |
See the base classes of the current class.
Definition at line 885 of file NPSMEFTd6.h.
Public Member Functions | |
| gslpp::complex | AH_f (const double tau) const |
| Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More... | |
| gslpp::complex | AH_W (const double tau) const |
| W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling. More... | |
| gslpp::complex | AHZga_f (const double tau, const double lambda) const |
| Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| gslpp::complex | AHZga_W (const double tau, const double lambda) const |
| W loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| virtual double | aPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| the angular parameter \(a\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More... | |
| virtual double | AuxObs_NP1 () const |
| Auxiliary observable AuxObs_NP1 (See code for details.) More... | |
| virtual double | AuxObs_NP10 () const |
| Auxiliary observable AuxObs_NP10 (See code for details.) More... | |
| virtual double | AuxObs_NP11 () const |
| Auxiliary observable AuxObs_NP11 (See code for details.) More... | |
| virtual double | AuxObs_NP12 () const |
| Auxiliary observable AuxObs_NP12 (See code for details.) More... | |
| virtual double | AuxObs_NP13 () const |
| Auxiliary observable AuxObs_NP13. More... | |
| virtual double | AuxObs_NP14 () const |
| Auxiliary observable AuxObs_NP14. More... | |
| virtual double | AuxObs_NP15 () const |
| Auxiliary observable AuxObs_NP15. More... | |
| virtual double | AuxObs_NP16 () const |
| Auxiliary observable AuxObs_NP16. More... | |
| virtual double | AuxObs_NP17 () const |
| Auxiliary observable AuxObs_NP17. More... | |
| virtual double | AuxObs_NP18 () const |
| Auxiliary observable AuxObs_NP18. More... | |
| virtual double | AuxObs_NP19 () const |
| Auxiliary observable AuxObs_NP19. More... | |
| virtual double | AuxObs_NP2 () const |
| Auxiliary observable AuxObs_NP2 (See code for details.) More... | |
| virtual double | AuxObs_NP20 () const |
| Auxiliary observable AuxObs_NP20. More... | |
| virtual double | AuxObs_NP3 () const |
| Auxiliary observable AuxObs_NP3 (See code for details.) More... | |
| virtual double | AuxObs_NP4 () const |
| Auxiliary observable AuxObs_NP4 (See code for details.) More... | |
| virtual double | AuxObs_NP5 () const |
| Auxiliary observable AuxObs_NP5 (See code for details.) More... | |
| virtual double | AuxObs_NP6 () const |
| Auxiliary observable AuxObs_NP6 (See code for details.) More... | |
| virtual double | AuxObs_NP7 () const |
| Auxiliary observable AuxObs_NP7 (See code for details.) More... | |
| virtual double | AuxObs_NP8 () const |
| Auxiliary observable AuxObs_NP8 (See code for details.) More... | |
| virtual double | AuxObs_NP9 () const |
| Auxiliary observable AuxObs_NP9 (See code for details.) More... | |
| virtual double | bPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| the angular parameter \(b\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More... | |
| virtual double | Br_H_exo () const |
| The branching ratio of the of the Higgs into exotic particles. More... | |
| virtual double | Br_H_inv () const |
| The branching ratio of the of the Higgs into invisible particles. More... | |
| virtual double | Br_H_inv_NP () const |
| The branching ratio of the of the Higgs into invisible particles (only invisible new particles). More... | |
| virtual double | BrHbbRatio () const |
| The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model. More... | |
| virtual double | BrHccRatio () const |
| The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model. More... | |
| virtual double | BrHgagaRatio () const |
| The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHggRatio () const |
| The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHmumuRatio () const |
| The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHtautauRatio () const |
| The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHtoinvRatio () const |
| The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHvisRatio () const |
| The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHWffRatio () const |
| The ratio of the Br \((H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| virtual double | BrHWjjRatio () const |
| The ratio of the Br \((H\to W j j)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHWlvRatio () const |
| The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHWW2l2vRatio () const |
| The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHWW4fRatio () const |
| The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| virtual double | BrHWW4jRatio () const |
| The ratio of the Br \((H\to WW^*\to 4j)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHWWRatio () const |
| The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZddRatio () const |
| The ratio of the Br \((H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZffRatio () const |
| The ratio of the Br \((H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| virtual double | BrHZgaeeRatio () const |
| The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZgallRatio () const |
| The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZgamumuRatio () const |
| The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZgaRatio () const |
| The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZllRatio () const |
| The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZuuRatio () const |
| The ratio of the Br \((H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZvvRatio () const |
| The ratio of the Br \((H\to Z\nu\nu)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ2e2muRatio () const |
| The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4dRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4eRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4fRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4lRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4muRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4uRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4vRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZRatio () const |
| The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model. More... | |
| virtual double | cgaga_HB () const |
| The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | cgg_HB () const |
| The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | cggEff_HB () const |
| The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual bool | CheckParameters (const std::map< std::string, double > &DPars) |
| A method to check if all the mandatory parameters for NPSMEFTd6 have been provided in model initialization. More... | |
| double | CLL_bottom () const |
| double | CLL_charm () const |
| double | CLL_down () const |
| double | CLL_mu () const |
| double | CLL_strange () const |
| double | CLL_tau () const |
| double | CLL_up () const |
| double | CLR_bottom () const |
| double | CLR_charm () const |
| double | CLR_down () const |
| double | CLR_mu () const |
| double | CLR_strange () const |
| double | CLR_tau () const |
| double | CLR_up () const |
| virtual double | computeGammaTotalRatio () const |
| The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. More... | |
| double | CRL_bottom () const |
| double | CRL_charm () const |
| double | CRL_down () const |
| double | CRL_mu () const |
| double | CRL_strange () const |
| double | CRL_tau () const |
| double | CRL_up () const |
| double | CRR_bottom () const |
| double | CRR_charm () const |
| double | CRR_down () const |
| double | CRR_mu () const |
| double | CRR_strange () const |
| double | CRR_tau () const |
| double | CRR_up () const |
| virtual double | cZBox_HB () const |
| The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | cZga_HB () const |
| The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | cZZ_HB () const |
| The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | deltaa0 () const |
| The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaa02 () const |
| The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaaMZ () const |
| The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaaMZ2 () const |
| The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaaSMZ () const |
| The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaaSMZ2 () const |
| The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltacZ_HB () const |
| The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | deltaG1_hWW () const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More... | |
| virtual double | deltaG1_hZA () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More... | |
| virtual double | deltaG1_hZARatio () const |
| The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual double | deltaG1_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More... | |
| virtual double | deltag1ZNP () const |
| The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\). More... | |
| virtual double | deltag1ZNPEff () const |
| The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More... | |
| virtual double | deltaG2_hWW () const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\). More... | |
| virtual double | deltaG2_hZA () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More... | |
| virtual double | deltaG2_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More... | |
| virtual double | deltaG3_hWW () const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More... | |
| virtual double | deltaG3_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More... | |
| double | deltag3G () const |
| The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\). More... | |
| gslpp::complex | deltaG_Aff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| gslpp::complex | deltaG_Gff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual double | deltaG_hAA () const |
| The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More... | |
| virtual double | deltaG_hAARatio () const |
| The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| gslpp::complex | deltaG_hAff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual gslpp::complex | deltaG_hff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More... | |
| gslpp::complex | deltaG_hGff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual double | deltaG_hgg () const |
| The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\). More... | |
| virtual double | deltaG_hggRatio () const |
| The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual double | deltaG_hhhRatio () const |
| The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More... | |
| gslpp::complex | deltaG_hZff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| gslpp::complex | deltaG_Zff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual double | deltaGA_f (const Particle p) const |
| New physics contribution to the neutral-current axial-vector coupling \(g_A^f\). More... | |
| virtual double | deltaGamma_W () const |
| The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\). More... | |
| virtual double | deltaGamma_Wff (const Particle fi, const Particle fj) const |
| The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More... | |
| double | deltaGammaHbbRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHbbRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHccRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHccRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHgagaRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHgagaRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHggRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More... | |
| double | deltaGammaHggRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHmumuRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHmumuRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHtautauRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHtautauRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWffRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWffRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWjjRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWjjRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWlvRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWlvRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWW2l2vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWW2l2vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWW4fRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWW4fRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWW4jRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWW4jRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWWRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWWRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZddRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZddRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZeeRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZeeRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZffRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZffRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZgaRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZgaRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZllRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZllRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZmumuRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZmumuRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZuuRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZuuRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZvvRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZvvRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ2e2muRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ2e2muRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4dRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4dRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4eRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4eRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4fRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4fRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4lRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4lRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4muRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4muRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4uRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4uRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| virtual double | deltaGammaTotalRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More... | |
| virtual double | deltaGammaTotalRatio1noError () const |
| The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. Neglecting SM theory errors. More... | |
| virtual double | deltaGammaTotalRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients. More... | |
| virtual double | DeltaGF () const |
| New physics contribution to the Fermi constant. More... | |
| double | deltaGL_f (const Particle p) const |
| New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More... | |
| virtual gslpp::complex | deltaGL_Wff (const Particle pbar, const Particle p) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| gslpp::complex | deltaGL_Wffh (const Particle pbar, const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| double | deltaGL_Zffh (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| virtual double | deltaGmu () const |
| The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaGmu2 () const |
| The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| double | deltaGR_f (const Particle p) const |
| New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More... | |
| virtual gslpp::complex | deltaGR_Wff (const Particle pbar, const Particle p) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| gslpp::complex | deltaGR_Wffh (const Particle pbar, const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| double | deltaGR_Zffh (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| virtual double | deltaGV_f (const Particle p) const |
| New physics contribution to the neutral-current vector coupling \(g_V^f\). More... | |
| virtual double | deltaGwd6 () const |
| The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\). More... | |
| virtual double | deltaGwd62 () const |
| The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\). More... | |
| virtual double | deltaGzd6 () const |
| The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\). More... | |
| virtual double | deltaGzd62 () const |
| The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\). More... | |
| virtual double | deltaKgammaNP () const |
| The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\). More... | |
| virtual double | deltaKgammaNPEff () const |
| The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More... | |
| virtual double | deltamb () const |
| The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltamb2 () const |
| The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltamc () const |
| The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltamc2 () const |
| The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaMh () const |
| The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaMh2 () const |
| The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltamt () const |
| The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltamt2 () const |
| The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltamtau () const |
| The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltamtau2 () const |
| The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaMwd6 () const |
| The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\). More... | |
| virtual double | deltaMwd62 () const |
| The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\). More... | |
| virtual double | deltaMz () const |
| The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaMz2 () const |
| The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltayb_HB () const |
| The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | deltayc_HB () const |
| The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | deltaymu_HB () const |
| The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | deltayt_HB () const |
| The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | deltaytau_HB () const |
| The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | dxseeWWdcos (const double sqrt_s, const double cos) const |
| The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle. More... | |
| virtual double | dxseeWWdcosBin (const double sqrt_s, const double cos1, const double cos2) const |
| The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle. More... | |
| gslpp::complex | f_triangle (const double tau) const |
| Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More... | |
| gslpp::complex | g_triangle (const double tau) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| double | GammaHbbRatio () const |
| The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. More... | |
| double | GammaHccRatio () const |
| The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. More... | |
| double | GammaHgagaRatio () const |
| The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. More... | |
| double | GammaHggRatio () const |
| The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. More... | |
| double | GammaHmumuRatio () const |
| The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. More... | |
| double | GammaHtautauRatio () const |
| The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. More... | |
| double | GammaHWffRatio () const |
| The ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| double | GammaHWjjRatio () const |
| The ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. More... | |
| double | GammaHWlvRatio () const |
| The ratio of the \(\Gamma(H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| double | GammaHWW2l2vRatio () const |
| The ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| double | GammaHWW4fRatio () const |
| The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| double | GammaHWW4jRatio () const |
| The ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. More... | |
| double | GammaHWWRatio () const |
| The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. More... | |
| double | GammaHZddRatio () const |
| The ratio of the \(\Gamma(H\to Zd d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More... | |
| double | GammaHZeeRatio () const |
| The ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. More... | |
| double | GammaHZffRatio () const |
| The ratio of the \(\Gamma(H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| double | GammaHZgaRatio () const |
| The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. More... | |
| double | GammaHZllRatio () const |
| The ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| double | GammaHZmumuRatio () const |
| The ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. More... | |
| double | GammaHZuuRatio () const |
| The ratio of the \(\Gamma(H\to Zu u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More... | |
| double | GammaHZvvRatio () const |
| The ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. More... | |
| double | GammaHZZ2e2muRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. More... | |
| double | GammaHZZ4dRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More... | |
| double | GammaHZZ4eRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More... | |
| double | GammaHZZ4fRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| double | GammaHZZ4lRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| double | GammaHZZ4muRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More... | |
| double | GammaHZZ4uRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More... | |
| double | GammaHZZ4vRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. More... | |
| double | GammaHZZRatio () const |
| The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. More... | |
| virtual double | GammaW () const |
| The total width of the \(W\) boson, \(\Gamma_W\). More... | |
| virtual double | GammaW (const Particle fi, const Particle fj) const |
| A partial decay width of the \(W\) boson decay into a SM fermion pair. More... | |
| double | getCed_1123 () const |
| Return NP coeff Ced_1123. More... | |
| double | getCed_2223 () const |
| Return NP coeff Ced_2223. More... | |
| double | getCeu_1133 () const |
| Return NP coeff Ceu_1133. More... | |
| double | getCeu_2233 () const |
| Return NP coeff Ceu_2233. More... | |
| double | getCHe_11 () const |
| Return NP coeff CHe_11. More... | |
| double | getCHe_22 () const |
| Return NP coeff CHe_22. More... | |
| double | getCHL1_11 () const |
| Return NP coeff CHL1_11. More... | |
| double | getCHL1_22 () const |
| Return NP coeff CHL1_22. More... | |
| double | getCHL3_11 () const |
| Return NP coeff CHL3_11. More... | |
| double | getCHL3_22 () const |
| Return NP coeff CHL3_22. More... | |
| double | getCLd_1123 () const |
| Return NP coeff CLd_1123. More... | |
| double | getCLd_2223 () const |
| Return NP coeff CLd_2223. More... | |
| double | getCLedQ_11 () const |
| Return NP coeff CLedq_11. More... | |
| double | getCLedQ_22 () const |
| Return NP coeff CLedq_22. More... | |
| double | getCLQ1_1123 () const |
| Return NP coeff CLQ1_1123. More... | |
| double | getCLQ1_2223 () const |
| Return NP coeff CLQ1_2223. More... | |
| double | getCLQ3_1123 () const |
| Return NP coeff CLQ3_1123. More... | |
| double | getCLQ3_2223 () const |
| Return NP coeff CLQ3_2223. More... | |
| double | getCLu_1133 () const |
| Return NP coeff CLu_1133. More... | |
| double | getCLu_2233 () const |
| Return NP coeff CLu_2233. More... | |
| double | getCpLedQ_11 () const |
| Return NP coeff CpLedq_11. More... | |
| double | getCpLedQ_22 () const |
| Return NP coeff CpLedq_22. More... | |
| double | getCQe_2311 () const |
| Return NP coeff CQe_2322. More... | |
| double | getCQe_2322 () const |
| Return NP coeff CQe_2322. More... | |
| double | getLambda_NP () const |
| Return Lambda_NP. More... | |
| virtual NPSMEFTd6Matching & | getMatching () const |
| A method to get the Matching object for this model. More... | |
| gslpp::complex | I_triangle_1 (const double tau, const double lambda) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| gslpp::complex | I_triangle_2 (const double tau, const double lambda) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| virtual double | kappaAeff () const |
| The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\). More... | |
| virtual double | kappabeff () const |
| The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\). More... | |
| virtual double | kappaceff () const |
| The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\). More... | |
| virtual double | kappaGeff () const |
| The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\). More... | |
| virtual double | kappamueff () const |
| The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\). More... | |
| virtual double | kappataueff () const |
| The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\). More... | |
| virtual double | kappaWeff () const |
| The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\). More... | |
| virtual double | kappaZAeff () const |
| The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\). More... | |
| virtual double | kappaZeff () const |
| The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\). More... | |
| virtual double | lambdaZNP () const |
| The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\). More... | |
| virtual double | lambz_HB () const |
| The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | mueeHvv (const double sqrt_s) const |
| The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeHvvPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueettH (const double sqrt_s) const |
| The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueettHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeWBF (const double sqrt_s) const |
| The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeWBFPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeWW (const double sqrt_s) const |
| The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeWWPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZBF (const double sqrt_s) const |
| The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZBFPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZH (const double sqrt_s) const |
| The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZllH (const double sqrt_s) const |
| The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZllHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZqqH (const double sqrt_s) const |
| The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZqqHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muepWBF (const double sqrt_s) const |
| The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muepZBF (const double sqrt_s) const |
| The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muggH (const double sqrt_s) const |
| The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muggHbb (const double sqrt_s) const |
| The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muggHgaga (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muggHH (const double sqrt_s) const |
| The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].) More... | |
| virtual double | muggHmumu (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muggHpttH (const double sqrt_s) const |
| The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muggHtautau (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muggHWW (const double sqrt_s) const |
| The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muggHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muggHZga (const double sqrt_s) const |
| The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muggHZZ (const double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muggHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | mummH (const double sqrt_s) const |
| The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mupTVppWZ (const double sqrt_s, const double pTV1, const double pTV2) const |
| The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class. More... | |
| virtual double | mutHq (const double sqrt_s) const |
| The ratio \(\mu_{tHq}\) between the t-q-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muTHUggHbb (const double sqrt_s) const |
| The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUggHgaga (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muTHUggHmumu (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUggHtautau (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUggHWW (const double sqrt_s) const |
| The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUggHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUggHZga (const double sqrt_s) const |
| The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUggHZgamumu (const double sqrt_s) const |
| The ratio \(\mu_{ggH,Z\gamma\to \gamma 2\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\to \gamma 2\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUggHZZ (const double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUggHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUggHZZ4mu (const double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ\to 4\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUttHbb (const double sqrt_s) const |
| The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUttHgaga (const double sqrt_s) const |
| The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muTHUttHmumu (const double sqrt_s) const |
| The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUttHtautau (const double sqrt_s) const |
| The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUttHWW (const double sqrt_s) const |
| The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUttHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUttHZga (const double sqrt_s) const |
| The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUttHZZ (const double sqrt_s) const |
| The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUttHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVBFBRinv (const double sqrt_s) const |
| The ratio \(\mu_{VBF}\) between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More... | |
| virtual double | muTHUVBFHbb (const double sqrt_s) const |
| The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVBFHgaga (const double sqrt_s) const |
| The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muTHUVBFHinv (const double sqrt_s) const |
| The ratio \(\mu_{VBF,inv}\) between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More... | |
| virtual double | muTHUVBFHmumu (const double sqrt_s) const |
| The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVBFHtautau (const double sqrt_s) const |
| The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVBFHWW (const double sqrt_s) const |
| The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVBFHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVBFHZga (const double sqrt_s) const |
| The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVBFHZZ (const double sqrt_s) const |
| The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVBFHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVHbb (const double sqrt_s) const |
| The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVHBRinv (const double sqrt_s) const |
| The ratio \(\mu_{VH}\) between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More... | |
| virtual double | muTHUVHgaga (const double sqrt_s) const |
| The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muTHUVHinv (const double sqrt_s) const |
| The ratio \(\mu_{VH,inv}\) between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More... | |
| virtual double | muTHUVHmumu (const double sqrt_s) const |
| The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVHtautau (const double sqrt_s) const |
| The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVHWW (const double sqrt_s) const |
| The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVHZga (const double sqrt_s) const |
| The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVHZZ (const double sqrt_s) const |
| The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUVHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUWHbb (const double sqrt_s) const |
| The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUWHgaga (const double sqrt_s) const |
| The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muTHUWHmumu (const double sqrt_s) const |
| The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUWHtautau (const double sqrt_s) const |
| The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUWHWW (const double sqrt_s) const |
| The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUWHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUWHZga (const double sqrt_s) const |
| The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUWHZZ (const double sqrt_s) const |
| The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUWHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUZHbb (const double sqrt_s) const |
| The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUZHgaga (const double sqrt_s) const |
| The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muTHUZHmumu (const double sqrt_s) const |
| The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUZHtautau (const double sqrt_s) const |
| The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUZHWW (const double sqrt_s) const |
| The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUZHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUZHZga (const double sqrt_s) const |
| The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUZHZZ (const double sqrt_s) const |
| The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muTHUZHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | muttH (const double sqrt_s) const |
| The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muttHbb (const double sqrt_s) const |
| The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muttHgaga (const double sqrt_s) const |
| The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muttHmumu (const double sqrt_s) const |
| The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muttHtautau (const double sqrt_s) const |
| The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muttHWW (const double sqrt_s) const |
| The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muttHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muttHZbbboost (const double sqrt_s) const |
| The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model. More... | |
| virtual double | muttHZga (const double sqrt_s) const |
| The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muttHZZ (const double sqrt_s) const |
| The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muttHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | muVBF (const double sqrt_s) const |
| The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muVBFgamma (const double sqrt_s) const |
| The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model. More... | |
| virtual double | muVBFHbb (const double sqrt_s) const |
| The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFHgaga (const double sqrt_s) const |
| The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muVBFHmumu (const double sqrt_s) const |
| The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFHtautau (const double sqrt_s) const |
| The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFHWW (const double sqrt_s) const |
| The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFHZga (const double sqrt_s) const |
| The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFHZZ (const double sqrt_s) const |
| The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFpVH (const double sqrt_s) const |
| The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muVH (const double sqrt_s) const |
| The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muVHbb (const double sqrt_s) const |
| The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muVHgaga (const double sqrt_s) const |
| The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muVHmumu (const double sqrt_s) const |
| The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muVHtautau (const double sqrt_s) const |
| The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muVHWW (const double sqrt_s) const |
| The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muVHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muVHZga (const double sqrt_s) const |
| The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muVHZZ (const double sqrt_s) const |
| The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muVHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | muWH (const double sqrt_s) const |
| The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muWHbb (const double sqrt_s) const |
| The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muWHgaga (const double sqrt_s) const |
| The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muWHmumu (const double sqrt_s) const |
| The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muWHtautau (const double sqrt_s) const |
| The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muWHWW (const double sqrt_s) const |
| The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muWHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muWHZga (const double sqrt_s) const |
| The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muWHZZ (const double sqrt_s) const |
| The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muWHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | muZH (const double sqrt_s) const |
| The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muZHbb (const double sqrt_s) const |
| The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muZHgaga (const double sqrt_s) const |
| The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muZHmumu (const double sqrt_s) const |
| The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muZHtautau (const double sqrt_s) const |
| The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muZHWW (const double sqrt_s) const |
| The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muZHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muZHZga (const double sqrt_s) const |
| The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muZHZZ (const double sqrt_s) const |
| The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muZHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | Mw () const |
| The mass of the \(W\) boson, \(M_W\). More... | |
| NPSMEFTd6 (const bool FlagLeptonUniversal_in=false, const bool FlagQuarkUniversal_in=false) | |
| Constructor. More... | |
| virtual double | obliqueS () const |
| The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).) More... | |
| virtual double | obliqueT () const |
| The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).) More... | |
| virtual double | obliqueU () const |
| The oblique parameter \(U\). More... | |
| virtual double | obliqueW () const |
| The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).) More... | |
| virtual double | obliqueY () const |
| The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).) More... | |
| virtual bool | PostUpdate () |
| The post-update method for NPSMEFTd6. More... | |
| virtual double | ppZHprobe (const double sqrt_s) const |
| The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class. More... | |
| virtual bool | setFlag (const std::string name, const bool value) |
| A method to set a flag of NPSMEFTd6. More... | |
| virtual double | STXS_ggH0j (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH1j_pTH_0_60 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH1j_pTH_120_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH1j_pTH_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH1j_pTH_60_120 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH2j_pTH_0_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH2j_pTH_0_60 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH2j_pTH_120_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH2j_pTH_200 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH2j_pTH_60_120 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_ggH_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual double | STXS_qqHll_pTV_0_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual double | STXS_qqHll_pTV_150_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual double | STXS_qqHll_pTV_150_250_0j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual double | STXS_qqHll_pTV_150_250_1j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual double | STXS_qqHll_pTV_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual double | STXS_qqHlv_pTV_0_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual double | STXS_qqHlv_pTV_0_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual double | STXS_qqHlv_pTV_150_250_0j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual double | STXS_qqHlv_pTV_150_250_1j (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual double | STXS_qqHlv_pTV_250 (const double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual double | STXS_qqHqq_pTj_200 (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual double | STXS_qqHqq_Rest (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual double | STXS_qqHqq_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual double | STXS_qqHqq_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual double | STXS_qqHqq_VBFtopo_Rest (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual double | STXS_qqHqq_VHtopo (const double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual double | STXS_ttHtH (const double sqrt_s) const |
| The STXS bin \( ttH + tH \). More... | |
| virtual double | STXS_WHqqHqq_pTj1_200 (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual double | STXS_WHqqHqq_Rest (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual double | STXS_WHqqHqq_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual double | STXS_WHqqHqq_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual double | STXS_WHqqHqq_VH2j (const double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual double | STXS_ZHqqHqq_pTj1_200 (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual double | STXS_ZHqqHqq_Rest (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual double | STXS_ZHqqHqq_VBFtopo_j3 (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual double | STXS_ZHqqHqq_VBFtopo_j3v (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual double | STXS_ZHqqHqq_VH2j (const double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual double | xseeWW (const double sqrt_s) const |
| Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\). More... | |
| Public Member Functions inherited from NPbase | |
| virtual double | A_f (const Particle f) const |
| The left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\mathcal{A}_f\). More... | |
| virtual double | AFB (const Particle f) const |
| The forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(A^f_{FB}\). More... | |
| virtual double | BR_Zf (const Particle f) const |
| The Branching ratio of the \(Z\) boson into a given fermion pair, \(BR_Z^{f}\). More... | |
| virtual double | cbminuscc () const |
| virtual double | cbminusctau () const |
| virtual double | ccminusctau () const |
| virtual double | cgaplusct () const |
| virtual double | cgminuscga () const |
| virtual double | cgplusct () const |
| virtual double | cVpluscb () const |
| virtual double | cVplusctau () const |
| virtual double | deltaA_f (const Particle f) const |
| The new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta \mathcal{A}_f\). More... | |
| virtual double | deltaAFB (const Particle f) const |
| The new physics contribution to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta A^f_{FB}\). More... | |
| virtual double | deltaGamma_Z () const |
| The new physics contribution to the total decay width of the \(Z\) boson, \(\delta \Gamma_Z\). More... | |
| virtual double | deltaGamma_Zf (const Particle f) const |
| The new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More... | |
| virtual double | deltaGamma_Zhad () const |
| The new physics contribution to the hadronic decay width of the \(Z\) boson, \(\delta \Gamma_{Z,had}\). More... | |
| virtual double | deltaN_nu () const |
| The new physics contribution to the number of neutrinos dervied from the \(Z\) pole measurements. More... | |
| virtual double | deltaR0_f (const Particle f) const |
| The new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More... | |
| virtual double | deltaR_inv () const |
| The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the \(Z\) boson, \(\delta R_{inv}\). More... | |
| virtual double | deltaSigmaHadron () const |
| The new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\delta \sigma_h^0\). More... | |
| virtual double | deltaSin2thetaEff_e () const |
| The new physics contribution to the effective electron/leptonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\rm lept}\) at the \(Z\) pole. More... | |
| virtual double | deltaSin2thetaEff_mu () const |
| The new physics contribution to the effective muonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\mu\mu}\) at the \(Z\) pole. More... | |
| virtual gslpp::complex | gA_f (const Particle f) const |
| The total (SM+NP) contribution to the neutral-current axial-vector coupling \(g_A^f\). More... | |
| virtual double | Gamma_had () const |
| The hadronic decay width of the \(Z\) boson, \(\Gamma_{Z,had}\). More... | |
| virtual double | Gamma_Z () const |
| The total decay width of the \(Z\) boson, \(\Gamma_Z\). More... | |
| virtual double | Gamma_Zf (const Particle f) const |
| The decay width of the \(Z\) boson into a given fermion pair, \(\Gamma_Z^{f}\). More... | |
| virtual StandardModel | getTrueSM () const |
| A method to return a StandardModel object from NPbase. More... | |
| virtual gslpp::complex | gV_f (const Particle f) const |
| The total (SM+NP) contribution to the neutral-current vector coupling \(g_V^f\). More... | |
| virtual gslpp::complex | kappaZ_f (const Particle f) const |
| The effective neutral-current coupling \(\kappa_Z^f\) including SM plus NP contributions. More... | |
| virtual double | muggHgagaInt (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. Includes interference effects with the background, following arXiv:1704.08259. More... | |
| virtual double | muppHmumu (const double sqrt_s) const |
| virtual double | muppHZga (const double sqrt_s) const |
| virtual double | N_nu () const |
| The number of neutrinos dervied from the \(Z\) pole measurements, \(N_{\nu}\). More... | |
| NPbase () | |
| The default constructor. More... | |
| virtual double | R0_f (const Particle f) const |
| The ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More... | |
| virtual double | R_inv () const |
| The ratio of the invisible and leptonic (electron) decay widths of the \(Z\) boson, \(R_{inv}\). More... | |
| virtual gslpp::complex | rhoZ_f (const Particle f) const |
| The effective neutral-current coupling \(\rho_Z^f\) including SM plus NP contributions. More... | |
| virtual double | sigma0_had () const |
| The cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\sigma_h^0\). More... | |
| virtual double | sin2thetaEff (const Particle f) const |
| The leptonic effective weak mixing angle \(\sin^2\theta_{\rm eff}^{\rm lept}\) at the the \(Z\) pole. More... | |
| virtual bool | Update (const std::map< std::string, double > &DPars) |
| The update method for NPbase. More... | |
| virtual double | UpperLimitZgammaA (const double sqrt_s) const |
| virtual double | UpperLimitZgammaA13 (const double sqrt_s) const |
| virtual double | UpperLimitZgammaC (const double sqrt_s) const |
| virtual double | UpperLimitZgammaC13 (const double sqrt_s) const |
| Public Member Functions inherited from StandardModel | |
| double | Ale (double mu, orders order, bool Nf_thr=true) const |
| The running electromagnetic coupling \(\alpha_e(\mu)\) in the \(\overline{MS}\) scheme. More... | |
| double | ale_OS (const double mu, orders order=FULLNLO) const |
| The running electromagnetic coupling \(\alpha(\mu)\) in the on-shell scheme. More... | |
| double | alphaMz () const |
| The electromagnetic coupling at the \(Z\)-mass scale, \(\alpha(M_Z^2)=\alpha/(1-\Delta\alpha(M_Z^2))\). More... | |
| double | Als (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) const |
| The running QCD coupling \(\alpha(\mu)\) in the \(\overline{MS}\) scheme including QED corrections. More... | |
| double | AlsByOrder (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) const |
| double | Alstilde5 (const double mu) const |
| The value of \(\frac{\alpha_s^{\mathrm{FULLNLO}}}{4\pi}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\) and full EW corrections. More... | |
| double | Beta_e (int nm, unsigned int nf) const |
| QED beta function coefficients - eq. (36) hep-ph/0512066. More... | |
| double | Beta_s (int nm, unsigned int nf) const |
| QCD beta function coefficients including QED corrections - eq. (36) hep-ph/0512066. More... | |
| double | c02 () const |
| The square of the cosine of the weak mixing angle \(c_0^2\) defined without weak radiative corrections. More... | |
| virtual bool | CheckFlags () const |
| A method to check the sanity of the set of model flags. More... | |
| bool | checkSMparamsForEWPO () |
| A method to check whether the parameters relevant to the EWPO are updated. More... | |
| double | computeBrHtobb () const |
| The Br \((H\to bb)\) in the Standard Model. More... | |
| double | computeBrHtocc () const |
| The Br \((H\to cc)\) in the Standard Model. More... | |
| double | computeBrHtogaga () const |
| The Br \((H\to\gamma\gamma)\) in the Standard Model. More... | |
| double | computeBrHtogg () const |
| The Br \((H\to gg)\) in the Standard Model. More... | |
| double | computeBrHtomumu () const |
| The Br \((H\to \mu\mu)\) in the Standard Model. More... | |
| double | computeBrHtoss () const |
| The Br \((H\to ss)\) in the Standard Model. More... | |
| double | computeBrHtotautau () const |
| The Br \((H\to \tau\tau)\) in the Standard Model. More... | |
| double | computeBrHtoWW () const |
| The Br \((H\to WW)\) in the Standard Model. More... | |
| double | computeBrHtoZga () const |
| The Br \((H\to Z\gamma)\) in the Standard Model. More... | |
| double | computeBrHtoZZ () const |
| The Br \((H\to ZZ)\) in the Standard Model. More... | |
| double | computeBrHtoZZinv () const |
| The Br \((H\to ZZ \to inv)\) in the Standard Model. More... | |
| void | ComputeDeltaR_rem (const double Mw_i, double DeltaR_rem[orders_EW_size]) const |
| A method to collect \(\Delta r_{\mathrm{rem}}\) computed via subclasses. More... | |
| void | ComputeDeltaRho (const double Mw_i, double DeltaRho[orders_EW_size]) const |
| A method to collect \(\Delta\rho\) computed via subclasses. More... | |
| double | computeGammaHgaga_tt () const |
| The top loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More... | |
| double | computeGammaHgaga_tW () const |
| The mixed \(t-W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More... | |
| double | computeGammaHgaga_WW () const |
| The \(W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More... | |
| double | computeGammaHgg_bb () const |
| The bottom loop contribution to \(H\to gg\) in the Standard Model. More... | |
| double | computeGammaHgg_tb () const |
| The top-bottom interference contribution to \(H\to gg\) in the Standard Model. More... | |
| double | computeGammaHgg_tt () const |
| The top loop contribution to \(H\to gg\) in the Standard Model. More... | |
| double | computeGammaHTotal () const |
| The Higgs total width in the Standard Model. More... | |
| double | computeGammaHZga_tt () const |
| The top loop contribution to \(H\to Z\gamma\) in the Standard Model. More... | |
| double | computeGammaHZga_tW () const |
| The mixed \(t-W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. More... | |
| double | computeGammaHZga_WW () const |
| The \(W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. Currently it returns the value of tab 41 in ref. [138]. More... | |
| double | computeSigmaggH (const double sqrt_s) const |
| The ggH cross section in the Standard Model. More... | |
| double | computeSigmaggH_bb (const double sqrt_s) const |
| The square of the bottom-quark contribution to the ggH cross section in the Standard Model. More... | |
| double | computeSigmaggH_tb (const double sqrt_s) const |
| The top-bottom interference contribution to the ggH cross section in the Standard Model. More... | |
| double | computeSigmaggH_tt (const double sqrt_s) const |
| The square of the top-quark contribution to the ggH cross section in the Standard Model. More... | |
| double | computeSigmattH (const double sqrt_s) const |
| The ttH production cross section in the Standard Model. More... | |
| double | computeSigmaVBF (const double sqrt_s) const |
| The VBF cross section in the Standard Model. More... | |
| double | computeSigmaWF (const double sqrt_s) const |
| The W fusion contribution \(\sigma_{WF}\) to higgs-production cross section in the Standard Model. More... | |
| double | computeSigmaWH (const double sqrt_s) const |
| The WH production cross section in the Standard Model. More... | |
| double | computeSigmaZF (const double sqrt_s) const |
| The Z fusion contribution \(\sigma_{ZF}\) to higgs-production cross section in the Standard Model. More... | |
| double | computeSigmaZH (const double sqrt_s) const |
| The ZH production cross section in the Standard Model. More... | |
| double | computeSigmaZWF (const double sqrt_s) const |
| The Z W interference fusion contribution \(\sigma_{ZWF}\) to higgs-production cross section in the Standard Model. More... | |
| virtual double | cW2 () const |
| virtual double | cW2 (const double Mw_i) const |
| The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as \(c_W^2\). More... | |
| double | DeltaAlpha () const |
| The total corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha(M_Z^2)\). More... | |
| double | DeltaAlphaL5q () const |
| The sum of the leptonic and the five-flavour hadronic corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha^{\ell+5q}(M_Z^2)\). More... | |
| double | DeltaAlphaLepton (const double s) const |
| Leptonic contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{lept}}(s)\). More... | |
| double | DeltaAlphaTop (const double s) const |
| Top-quark contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{top}}(s)\). More... | |
| virtual gslpp::complex | deltaKappaZ_f (const Particle f) const |
| Flavour non-universal vertex corrections to \(\kappa_Z^l\), denoted by \(\Delta\kappa_Z^l\). More... | |
| virtual double | DeltaR () const |
| The SM prediction for \(\Delta r\) derived from that for the \(W\) boson mass. More... | |
| virtual double | DeltaRbar () const |
| The SM prediction for \(\Delta \overline{r}\) derived from that for the \(W\)-boson mass. More... | |
| virtual gslpp::complex | deltaRhoZ_f (const Particle f) const |
| Flavour non-universal vertex corrections to \(\rho_Z^l\), denoted by \(\Delta\rho_Z^l\). More... | |
| virtual double | epsilon1 () const |
| The SM contribution to the epsilon parameter \(\varepsilon_1\). More... | |
| virtual double | epsilon2 () const |
| The SM contribution to the epsilon parameter \(\varepsilon_2\). More... | |
| virtual double | epsilon3 () const |
| The SM contribution to the epsilon parameter \(\varepsilon_3\). More... | |
| virtual double | epsilonb () const |
| The SM contribution to the epsilon parameter \(\varepsilon_b\). More... | |
| virtual double | Gamma_inv () const |
| The invisible partial decay width of the \(Z\) boson, \(\Gamma_{\mathrm{inv}}\). More... | |
| virtual double | GammaZ (const Particle f) const |
| The \(Z\to \ell\bar{\ell}\) partial decay width, \(\Gamma_\ell\). More... | |
| double | getAle () const |
| A get method to retrieve the fine-structure constant \(\alpha\). More... | |
| double | getAlsMz () const |
| A get method to access the value of \(\alpha_s(M_Z)\). More... | |
| virtual double | getCBd () const |
| The ratio of the absolute value of the $B_d$ mixing amplitude over the Standard Model value. More... | |
| virtual double | getCBs () const |
| The ratio of the absolute value of the $B_s$ mixing amplitude over the Standard Model value. More... | |
| virtual double | getCCC1 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual double | getCCC2 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual double | getCCC3 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual double | getCCC4 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual double | getCCC5 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual double | getCDMK () const |
| The ratio of the real part of the $K$ mixing amplitude over the Standard Model value. More... | |
| virtual double | getCepsK () const |
| The ratio of the imaginary part of the $K$ mixing amplitude over the Standard Model value. More... | |
| CKM | getCKM () const |
| A get method to retrieve the member object of type CKM. More... | |
| double | getDAle5Mz () const |
| A get method to retrieve the five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More... | |
| double | getDelGammaZ () const |
| A get method to retrieve the theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\). More... | |
| double | getDelMw () const |
| A get method to retrieve the theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\). More... | |
| double | getDelR0b () const |
| A get method to retrieve the theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More... | |
| double | getDelR0c () const |
| A get method to retrieve the theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More... | |
| double | getDelR0l () const |
| A get method to retrieve the theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More... | |
| double | getDelSigma0H () const |
| A get method to retrieve the theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\). More... | |
| double | getDelSin2th_b () const |
| A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More... | |
| double | getDelSin2th_l () const |
| A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More... | |
| double | getDelSin2th_q () const |
| A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More... | |
| std::string | getFlagKappaZ () const |
| A method to retrieve the model flag KappaZ. More... | |
| std::string | getFlagMw () const |
| A method to retrieve the model flag Mw. More... | |
| std::string | getFlagRhoZ () const |
| A method to retrieve the model flag RhoZ. More... | |
| const Flavour & | getFlavour () const |
| double | getGF () const |
| A get method to retrieve the Fermi constant \(G_\mu\). More... | |
| int | getIterationNo () const |
| Particle | getLeptons (const QCD::lepton p) const |
| A get method to retrieve the member object of a lepton. More... | |
| virtual double | getMHl () const |
| A get method to retrieve the Higgs mass \(m_h\). More... | |
| virtual double | getmq (const QCD::quark q, const double mu) const |
| double | getMuw () const |
| A get method to retrieve the matching scale \(\mu_W\) around the weak scale. More... | |
| EWSMApproximateFormulae * | getMyApproximateFormulae () const |
| A get method to retrieve the member pointer of type EWSMApproximateFormulae. More... | |
| EWSMcache * | getMyEWSMcache () const |
| A get method to retrieve the member pointer of type EWSMcache. More... | |
| LeptonFlavour * | getMyLeptonFlavour () const |
| EWSMOneLoopEW * | getMyOneLoopEW () const |
| A get method to retrieve the member pointer of type EWSMOneLoopEW,. More... | |
| EWSMThreeLoopEW * | getMyThreeLoopEW () const |
| EWSMThreeLoopEW2QCD * | getMyThreeLoopEW2QCD () const |
| EWSMThreeLoopQCD * | getMyThreeLoopQCD () const |
| EWSMTwoFermionsLEP2 * | getMyTwoFermionsLEP2 () const |
| A get method to retrieve the member pointer of type EWSMTwoFermionsLEP2. More... | |
| EWSMTwoLoopEW * | getMyTwoLoopEW () const |
| EWSMTwoLoopQCD * | getMyTwoLoopQCD () const |
| double | getMz () const |
| A get method to access the mass of the \(Z\) boson \(M_Z\). More... | |
| virtual double | getPhiBd () const |
| Half the relative phase of the $B_d$ mixing amplitude w.r.t. the Standard Model one. More... | |
| virtual double | getPhiBs () const |
| Half the relative phase of the $B_s$ mixing amplitude w.r.t. the Standard Model one. More... | |
| gslpp::matrix< gslpp::complex > | getUPMNS () const |
| A get method to retrieve the object of the PMNS matrix. More... | |
| gslpp::matrix< gslpp::complex > | getVCKM () const |
| A get method to retrieve the CKM matrix. More... | |
| gslpp::matrix< gslpp::complex > | getYd () const |
| A get method to retrieve the Yukawa matrix of the down-type quarks, \(Y_d\). More... | |
| gslpp::matrix< gslpp::complex > | getYe () const |
| A get method to retrieve the Yukawa matrix of the charged leptons, \(Y_e\). More... | |
| gslpp::matrix< gslpp::complex > | getYn () const |
| A get method to retrieve the Yukawa matrix of the neutrinos, \(Y_\nu\). More... | |
| gslpp::matrix< gslpp::complex > | getYu () const |
| A get method to retrieve the Yukawa matrix of the up-type quarks, \(Y_u\). More... | |
| virtual bool | Init (const std::map< std::string, double > &DPars) |
| A method to initialize the model parameters. More... | |
| virtual bool | InitializeModel () |
| A method to initialize the model. More... | |
| bool | IsFlagNoApproximateGammaZ () const |
| A method to retrieve the model flag NoApproximateGammaZ. More... | |
| bool | IsFlagWithoutNonUniversalVC () const |
| A method to retrieve the model flag WithoutNonUniversalVC. More... | |
| virtual double | LEP2AFBbottom (const double s) const |
| virtual double | LEP2AFBcharm (const double s) const |
| virtual double | LEP2AFBmu (const double s) const |
| virtual double | LEP2AFBtau (const double s) const |
| virtual double | LEP2Rbottom (const double s) const |
| virtual double | LEP2Rcharm (const double s) const |
| virtual double | LEP2sigmaBottom (const double s) const |
| virtual double | LEP2sigmaCharm (const double s) const |
| virtual double | LEP2sigmaHadron (const double s) const |
| virtual double | LEP2sigmaMu (const double s) const |
| virtual double | LEP2sigmaTau (const double s) const |
| virtual double | Mw_tree () const |
| The tree-level mass of the \(W\) boson, \(M_W^{\mathrm{tree}}\). More... | |
| double | MwbarFromMw (const double Mw) const |
| A method to convert the \(W\)-boson mass in the experimental/running-width scheme to that in the complex-pole/fixed-width scheme. More... | |
| double | MwFromMwbar (const double Mwbar) const |
| A method to convert the \(W\)-boson mass in the complex-pole/fixed-width scheme to that in the experimental/running-width scheme. More... | |
| double | Mzbar () const |
| The \(Z\)-boson mass \(\overline{M}_Z\) in the complex-pole/fixed-width scheme. More... | |
| virtual bool | PreUpdate () |
| The pre-update method for StandardModel. More... | |
| virtual double | rho_GammaW (const Particle fi, const Particle fj) const |
| EW radiative corrections to the width of \(W \to f_i \bar{f}_j\), denoted as \(\rho^W_{ij}\). More... | |
| double | s02 () const |
| The square of the sine of the weak mixing angle \(s_0^2\) defined without weak radiative corrections. More... | |
| void | setFlagCacheInStandardModel (bool FlagCacheInStandardModel) |
| A set method to change the model flag CacheInStandardModel of StandardModel. More... | |
| void | setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ) |
| bool | setFlagSigmaForAFB (const bool flagSigmaForAFB_i) |
| bool | setFlagSigmaForR (const bool flagSigmaForR_i) |
| virtual bool | setFlagStr (const std::string name, const std::string value) |
| A method to set a flag of StandardModel. More... | |
| StandardModel () | |
| The default constructor. More... | |
| double | sW2 () const |
| virtual double | sW2 (const double Mw_i) const |
| The square of the sine of the weak mixing angle in the on-shell scheme, denoted as \(s_W^2\). More... | |
| virtual double | v () const |
| The Higgs vacuum expectation value. More... | |
| virtual | ~StandardModel () |
| The default destructor. More... | |
| Public Member Functions inherited from QCD | |
| double | AboveTh (const double mu) const |
| The active flavour threshold above the scale \(\mu\) as defined in QCD::Thresholds(). More... | |
| void | addParameters (std::vector< std::string > params_i) |
| A method to add parameters that are specific to only one set of observables. More... | |
| virtual double | Als (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const |
| double | Als4 (const double mu) const |
| The value of \(\alpha_s^{\mathrm{FULLNLO}}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\). More... | |
| virtual double | AlsByOrder (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const |
| double | AlsOLD (const double mu, const orders order=FULLNLO) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More... | |
| double | AlsWithInit (const double mu, const double alsi, const double mu_i, const orders order) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) from \(\alpha_s(\mu_i)\) in the \(\overline{\mathrm{MS}}\) scheme, where it is forbidden to across a flavour threshold in the RG running from \(\mu_i\) to \(\mu\). More... | |
| double | AlsWithLambda (const double mu, const orders order) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme with the use of \(\Lambda_{\rm QCD}\). More... | |
| double | BelowTh (const double mu) const |
| The active flavour threshold below the scale \(\mu\) as defined in QCD::Thresholds(). More... | |
| double | Beta0 (const double nf) const |
| The \(\beta_0(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| double | Beta1 (const double nf) const |
| The \(\beta_1(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| double | Beta2 (const double nf) const |
| The \(\beta_2(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| double | Beta3 (const double nf) const |
| The \(\beta_3(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| void | CacheShift (double cache[][5], int n) const |
| A member used to manage the caching for this class. More... | |
| void | CacheShift (int cache[][5], int n) const |
| orders | FullOrder (orders order) const |
| Return the FULLORDER enum corresponding to order. More... | |
| double | Gamma0 (const double nf) const |
| The \(\gamma_0\) coefficient used to compute the running of a mass. More... | |
| double | Gamma1 (const double nf) const |
| The \(\gamma_1\) coefficient used to compute the running of a mass. More... | |
| double | Gamma2 (const double nf) const |
| The \(\gamma_2\) coefficient used to compute the running of a mass. More... | |
| double | getAlsM () const |
| A get method to access the value of \(\alpha_s(M_{\alpha_s})\). More... | |
| BParameter | getBBd () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_d\) meson system. More... | |
| BParameter | getBBs () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_s\) meson system. More... | |
| BParameter | getBD () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta c = 2\) process in the \(D^0\) meson system. More... | |
| BParameter | getBK () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta s = 2\) process in the \(K^0\) meson system. More... | |
| BParameter | getBKd1 () const |
| BParameter | getBKd3 () const |
| double | getCF () const |
| A get method to access the Casimir factor of QCD. More... | |
| double | getMAls () const |
| A get method to access the mass scale \(M_{\alpha_s}\) at which the strong coupling constant measurement is provided. More... | |
| Meson | getMesons (const QCD::meson m) const |
| A get method to access a meson as an object of the type Meson. More... | |
| double | getMtpole () const |
| A get method to access the pole mass of the top quark. More... | |
| double | getMub () const |
| A get method to access the threshold between five- and four-flavour theory in GeV. More... | |
| double | getMuc () const |
| A get method to access the threshold between four- and three-flavour theory in GeV. More... | |
| double | getMut () const |
| A get method to access the threshold between six- and five-flavour theory in GeV. More... | |
| double | getNc () const |
| A get method to access the number of colours \(N_c\). More... | |
| double | getOptionalParameter (std::string name) const |
| A method to get parameters that are specific to only one set of observables. More... | |
| Particle | getQuarks (const QCD::quark q) const |
| A get method to access a quark as an object of the type Particle. More... | |
| std::vector< std::string > | getUnknownParameters () |
| A method to get the vector of the parameters that have been specified in the configuration file but not being used. More... | |
| void | initializeBParameter (std::string name_i) const |
| A method to initialize B Parameter and the corresponding meson. More... | |
| void | initializeMeson (QCD::meson meson_i) const |
| A method to initialize a meson. More... | |
| double | logLambda (const double nf, orders order) const |
| Computes \(\ln\Lambda_\mathrm{QCD}\) with nf flavours in GeV. More... | |
| double | Mbar2Mp (const double mbar, const orders order=FULLNNLO) const |
| Converts the \(\overline{\mathrm{MS}}\) mass \(m(m)\) to the pole mass. More... | |
| double | Mp2Mbar (const double mp, const orders order=FULLNNLO) const |
| Converts a quark pole mass to the corresponding \(\overline{\mathrm{MS}}\) mass \(m(m)\). More... | |
| double | Mrun (const double mu, const double m, const orders order=FULLNNLO) const |
| Computes a running quark mass \(m(\mu)\) from \(m(m)\). More... | |
| double | Mrun (const double mu_f, const double mu_i, const double m, const orders order=FULLNNLO) const |
| Runs a quark mass from \(\mu_i\) to \(\mu_f\). More... | |
| double | Mrun4 (const double mu_f, const double mu_i, const double m) const |
| The running of a mass with the number of flavours \(n_f = 4\). More... | |
| double | MS2DRqmass (const double MSbar) const |
| Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More... | |
| double | MS2DRqmass (const double MSscale, const double MSbar) const |
| Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More... | |
| double | Nf (const double mu) const |
| The number of active flavour at scale \(\mu\). More... | |
| double | NfThresholdCorrections (double mu, double M, double als, int nf, orders order) const |
| Threshold corrections in matching \(\alpha_s(n_f+1)\) with \(\alpha_s(n_f)\) from eq. (34) of hep-ph/0512060. More... | |
| std::string | orderToString (const orders order) const |
| Converts an object of the enum type "orders" to the corresponding string. More... | |
| QCD () | |
| Constructor. More... | |
| void | setNc (double Nc) |
| A set method to change the number of colours \(N_c\). More... | |
| void | setOptionalParameter (std::string name, double value) |
| A method to set the parameter value for the parameters that are specific to only one set of observables. More... | |
| double | Thresholds (const int i) const |
| For accessing the active flavour threshold scales. More... | |
| Public Member Functions inherited from Model | |
| void | addMissingModelParameter (const std::string &missingParameterName) |
| std::vector< std::string > | getmissingModelParameters () |
| unsigned int | getMissingModelParametersCount () |
| std::string | getModelName () const |
| A method to fetch the name of the model. More... | |
| const double & | getModelParam (std::string name) const |
| bool | isModelFWC_DF2 () const |
| bool | isModelGeneralTHDM () const |
| bool | isModelGeorgiMachacek () const |
| bool | IsModelInitialized () const |
| A method to check if the model is initialized. More... | |
| bool | isModelLinearized () const |
| bool | isModelParam (std::string name) const |
| bool | isModelSUSY () const |
| bool | isModelTHDM () const |
| bool | isModelTHDMW () const |
| bool | IsUpdateError () const |
| A method to check if there was any error in the model update process. More... | |
| Model () | |
| The default constructor. More... | |
| void | raiseMissingModelParameterCount () |
| void | setModelFWC_DF2 () |
| void | setModelGeneralTHDM () |
| void | setModelGeorgiMachacek () |
| void | setModelInitialized (bool ModelInitialized) |
| A set method to fix the failure or success of the initialization of the model. More... | |
| void | setModelLinearized (bool linearized=true) |
| void | setModelName (const std::string name) |
| A method to set the name of the model. More... | |
| void | setModelSUSY () |
| void | setModelTHDM () |
| void | setModelTHDMW () |
| void | setSliced (bool Sliced) |
| void | setUpdateError (bool UpdateError) |
| A set method to fix the update status as success or failure. More... | |
| virtual | ~Model () |
| The default destructor. More... | |
Static Public Attributes | |
| static const int | NNPSMEFTd6Vars = 506 |
| The number of the model parameters in NPSMEFTd6. More... | |
| static const int | NNPSMEFTd6Vars_LFU_QFU = 260 |
| The number of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities. More... | |
| static const std::string | NPSMEFTd6Vars [NNPSMEFTd6Vars] |
| A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=false. More... | |
| static const std::string | NPSMEFTd6Vars_LFU_QFU [NNPSMEFTd6Vars_LFU_QFU] |
| A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=false. More... | |
| static const std::string | NPSMEFTd6VarsRot [NNPSMEFTd6Vars] |
| A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=true. More... | |
| static const std::string | NPSMEFTd6VarsRot_LFU_QFU [NNPSMEFTd6Vars_LFU_QFU] |
| A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=true. More... | |
| Static Public Attributes inherited from StandardModel | |
| static const double | GeVminus2_to_nb = 389379.338 |
| static const double | Mw_error = 0.00001 |
| The target accuracy of the iterative calculation of the \(W\)-boson mass in units of GeV. More... | |
| static const int | NSMvars = 26 |
| The number of the model parameters in StandardModel. More... | |
| static const int | NumSMParamsForEWPO = 33 |
| The number of the SM parameters that are relevant to the EW precision observables. More... | |
| static std::string | SMvars [NSMvars] |
| A string array containing the labels of the model parameters in StandardModel. More... | |
| Static Public Attributes inherited from QCD | |
| static const int | NQCDvars = 11 |
| The number of model parameters in QCD. More... | |
| static std::string | QCDvars [NQCDvars] |
| An array containing the labels under which all QCD parameters are stored in a vector of ModelParameter via InputParser::ReadParameters(). More... | |
Protected Member Functions | |
| gslpp::complex | CfB_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f. More... | |
| gslpp::complex | CfG_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f. More... | |
| gslpp::complex | CfH_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f. More... | |
| gslpp::complex | CfW_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) corresponding to particle f. More... | |
| double | CHF1_diag (const Particle F) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F. More... | |
| double | CHF3_diag (const Particle F) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F. More... | |
| double | CHf_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f. More... | |
| gslpp::complex | CHud_diag (const Particle u) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{Hud}\) corresponding to particle f. More... | |
| virtual void | setParameter (const std::string name, const double &value) |
| A method to set the value of a parameter of the model. More... | |
| Protected Member Functions inherited from StandardModel | |
| double | AFB_NoISR_l (const QCD::lepton l_flavor, const double s) const |
| double | AFB_NoISR_q (const QCD::quark q_flavor, const double s) const |
| bool | checkEWPOscheme (const std::string scheme) const |
| A method to check if a given scheme name in string form is valid. More... | |
| virtual void | computeCKM () |
| The method to compute the CKM matrix. More... | |
| virtual void | computeYukawas () |
| The method to compute the Yukawa matrices. More... | |
| double | Delta_EWQCD (const QCD::quark q) const |
| The non-factorizable EW-QCD corrections to the partial widths for \(Z\to q\bar{q}\), denoted as \(\Delta_{\mathrm{EW/QCD}}\). More... | |
| double | getIntegrand_AFBnumeratorWithISR_bottom133 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom167 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom172 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom183 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom189 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom192 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom196 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom200 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom202 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom205 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom207 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm133 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm167 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm172 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm183 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm189 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm192 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm196 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm200 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm202 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm205 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm207 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu130 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu136 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu161 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu172 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu183 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu189 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu192 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu196 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu200 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu202 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu205 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu207 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau130 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau136 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau161 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau172 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau183 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau189 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau192 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau196 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau200 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau202 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau205 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau207 (double x) const |
| double | getIntegrand_dsigmaBox_bottom130 (double x) const |
| double | getIntegrand_dsigmaBox_bottom133 (double x) const |
| double | getIntegrand_dsigmaBox_bottom136 (double x) const |
| double | getIntegrand_dsigmaBox_bottom161 (double x) const |
| double | getIntegrand_dsigmaBox_bottom167 (double x) const |
| double | getIntegrand_dsigmaBox_bottom172 (double x) const |
| double | getIntegrand_dsigmaBox_bottom183 (double x) const |
| double | getIntegrand_dsigmaBox_bottom189 (double x) const |
| double | getIntegrand_dsigmaBox_bottom192 (double x) const |
| double | getIntegrand_dsigmaBox_bottom196 (double x) const |
| double | getIntegrand_dsigmaBox_bottom200 (double x) const |
| double | getIntegrand_dsigmaBox_bottom202 (double x) const |
| double | getIntegrand_dsigmaBox_bottom205 (double x) const |
| double | getIntegrand_dsigmaBox_bottom207 (double x) const |
| double | getIntegrand_dsigmaBox_charm130 (double x) const |
| double | getIntegrand_dsigmaBox_charm133 (double x) const |
| double | getIntegrand_dsigmaBox_charm136 (double x) const |
| double | getIntegrand_dsigmaBox_charm161 (double x) const |
| double | getIntegrand_dsigmaBox_charm167 (double x) const |
| double | getIntegrand_dsigmaBox_charm172 (double x) const |
| double | getIntegrand_dsigmaBox_charm183 (double x) const |
| double | getIntegrand_dsigmaBox_charm189 (double x) const |
| double | getIntegrand_dsigmaBox_charm192 (double x) const |
| double | getIntegrand_dsigmaBox_charm196 (double x) const |
| double | getIntegrand_dsigmaBox_charm200 (double x) const |
| double | getIntegrand_dsigmaBox_charm202 (double x) const |
| double | getIntegrand_dsigmaBox_charm205 (double x) const |
| double | getIntegrand_dsigmaBox_charm207 (double x) const |
| double | getIntegrand_dsigmaBox_down130 (double x) const |
| double | getIntegrand_dsigmaBox_down133 (double x) const |
| double | getIntegrand_dsigmaBox_down136 (double x) const |
| double | getIntegrand_dsigmaBox_down161 (double x) const |
| double | getIntegrand_dsigmaBox_down167 (double x) const |
| double | getIntegrand_dsigmaBox_down172 (double x) const |
| double | getIntegrand_dsigmaBox_down183 (double x) const |
| double | getIntegrand_dsigmaBox_down189 (double x) const |
| double | getIntegrand_dsigmaBox_down192 (double x) const |
| double | getIntegrand_dsigmaBox_down196 (double x) const |
| double | getIntegrand_dsigmaBox_down200 (double x) const |
| double | getIntegrand_dsigmaBox_down202 (double x) const |
| double | getIntegrand_dsigmaBox_down205 (double x) const |
| double | getIntegrand_dsigmaBox_down207 (double x) const |
| double | getIntegrand_dsigmaBox_mu130 (double x) const |
| double | getIntegrand_dsigmaBox_mu133 (double x) const |
| double | getIntegrand_dsigmaBox_mu136 (double x) const |
| double | getIntegrand_dsigmaBox_mu161 (double x) const |
| double | getIntegrand_dsigmaBox_mu167 (double x) const |
| double | getIntegrand_dsigmaBox_mu172 (double x) const |
| double | getIntegrand_dsigmaBox_mu183 (double x) const |
| double | getIntegrand_dsigmaBox_mu189 (double x) const |
| double | getIntegrand_dsigmaBox_mu192 (double x) const |
| double | getIntegrand_dsigmaBox_mu196 (double x) const |
| double | getIntegrand_dsigmaBox_mu200 (double x) const |
| double | getIntegrand_dsigmaBox_mu202 (double x) const |
| double | getIntegrand_dsigmaBox_mu205 (double x) const |
| double | getIntegrand_dsigmaBox_mu207 (double x) const |
| double | getIntegrand_dsigmaBox_strange130 (double x) const |
| double | getIntegrand_dsigmaBox_strange133 (double x) const |
| double | getIntegrand_dsigmaBox_strange136 (double x) const |
| double | getIntegrand_dsigmaBox_strange161 (double x) const |
| double | getIntegrand_dsigmaBox_strange167 (double x) const |
| double | getIntegrand_dsigmaBox_strange172 (double x) const |
| double | getIntegrand_dsigmaBox_strange183 (double x) const |
| double | getIntegrand_dsigmaBox_strange189 (double x) const |
| double | getIntegrand_dsigmaBox_strange192 (double x) const |
| double | getIntegrand_dsigmaBox_strange196 (double x) const |
| double | getIntegrand_dsigmaBox_strange200 (double x) const |
| double | getIntegrand_dsigmaBox_strange202 (double x) const |
| double | getIntegrand_dsigmaBox_strange205 (double x) const |
| double | getIntegrand_dsigmaBox_strange207 (double x) const |
| double | getIntegrand_dsigmaBox_tau130 (double x) const |
| double | getIntegrand_dsigmaBox_tau133 (double x) const |
| double | getIntegrand_dsigmaBox_tau136 (double x) const |
| double | getIntegrand_dsigmaBox_tau161 (double x) const |
| double | getIntegrand_dsigmaBox_tau167 (double x) const |
| double | getIntegrand_dsigmaBox_tau172 (double x) const |
| double | getIntegrand_dsigmaBox_tau183 (double x) const |
| double | getIntegrand_dsigmaBox_tau189 (double x) const |
| double | getIntegrand_dsigmaBox_tau192 (double x) const |
| double | getIntegrand_dsigmaBox_tau196 (double x) const |
| double | getIntegrand_dsigmaBox_tau200 (double x) const |
| double | getIntegrand_dsigmaBox_tau202 (double x) const |
| double | getIntegrand_dsigmaBox_tau205 (double x) const |
| double | getIntegrand_dsigmaBox_tau207 (double x) const |
| double | getIntegrand_dsigmaBox_up130 (double x) const |
| double | getIntegrand_dsigmaBox_up133 (double x) const |
| double | getIntegrand_dsigmaBox_up136 (double x) const |
| double | getIntegrand_dsigmaBox_up161 (double x) const |
| double | getIntegrand_dsigmaBox_up167 (double x) const |
| double | getIntegrand_dsigmaBox_up172 (double x) const |
| double | getIntegrand_dsigmaBox_up183 (double x) const |
| double | getIntegrand_dsigmaBox_up189 (double x) const |
| double | getIntegrand_dsigmaBox_up192 (double x) const |
| double | getIntegrand_dsigmaBox_up196 (double x) const |
| double | getIntegrand_dsigmaBox_up200 (double x) const |
| double | getIntegrand_dsigmaBox_up202 (double x) const |
| double | getIntegrand_dsigmaBox_up205 (double x) const |
| double | getIntegrand_dsigmaBox_up207 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom130 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom133 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom136 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom161 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom167 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom172 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom183 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom189 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom192 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom196 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom200 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom202 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom205 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom207 (double x) const |
| double | getIntegrand_sigmaWithISR_charm130 (double x) const |
| double | getIntegrand_sigmaWithISR_charm133 (double x) const |
| double | getIntegrand_sigmaWithISR_charm136 (double x) const |
| double | getIntegrand_sigmaWithISR_charm161 (double x) const |
| double | getIntegrand_sigmaWithISR_charm167 (double x) const |
| double | getIntegrand_sigmaWithISR_charm172 (double x) const |
| double | getIntegrand_sigmaWithISR_charm183 (double x) const |
| double | getIntegrand_sigmaWithISR_charm189 (double x) const |
| double | getIntegrand_sigmaWithISR_charm192 (double x) const |
| double | getIntegrand_sigmaWithISR_charm196 (double x) const |
| double | getIntegrand_sigmaWithISR_charm200 (double x) const |
| double | getIntegrand_sigmaWithISR_charm202 (double x) const |
| double | getIntegrand_sigmaWithISR_charm205 (double x) const |
| double | getIntegrand_sigmaWithISR_charm207 (double x) const |
| double | getIntegrand_sigmaWithISR_down130 (double x) const |
| double | getIntegrand_sigmaWithISR_down133 (double x) const |
| double | getIntegrand_sigmaWithISR_down136 (double x) const |
| double | getIntegrand_sigmaWithISR_down161 (double x) const |
| double | getIntegrand_sigmaWithISR_down167 (double x) const |
| double | getIntegrand_sigmaWithISR_down172 (double x) const |
| double | getIntegrand_sigmaWithISR_down183 (double x) const |
| double | getIntegrand_sigmaWithISR_down189 (double x) const |
| double | getIntegrand_sigmaWithISR_down192 (double x) const |
| double | getIntegrand_sigmaWithISR_down196 (double x) const |
| double | getIntegrand_sigmaWithISR_down200 (double x) const |
| double | getIntegrand_sigmaWithISR_down202 (double x) const |
| double | getIntegrand_sigmaWithISR_down205 (double x) const |
| double | getIntegrand_sigmaWithISR_down207 (double x) const |
| double | getIntegrand_sigmaWithISR_mu130 (double x) const |
| double | getIntegrand_sigmaWithISR_mu136 (double x) const |
| double | getIntegrand_sigmaWithISR_mu161 (double x) const |
| double | getIntegrand_sigmaWithISR_mu172 (double x) const |
| double | getIntegrand_sigmaWithISR_mu183 (double x) const |
| double | getIntegrand_sigmaWithISR_mu189 (double x) const |
| double | getIntegrand_sigmaWithISR_mu192 (double x) const |
| double | getIntegrand_sigmaWithISR_mu196 (double x) const |
| double | getIntegrand_sigmaWithISR_mu200 (double x) const |
| double | getIntegrand_sigmaWithISR_mu202 (double x) const |
| double | getIntegrand_sigmaWithISR_mu205 (double x) const |
| double | getIntegrand_sigmaWithISR_mu207 (double x) const |
| double | getIntegrand_sigmaWithISR_strange130 (double x) const |
| double | getIntegrand_sigmaWithISR_strange133 (double x) const |
| double | getIntegrand_sigmaWithISR_strange136 (double x) const |
| double | getIntegrand_sigmaWithISR_strange161 (double x) const |
| double | getIntegrand_sigmaWithISR_strange167 (double x) const |
| double | getIntegrand_sigmaWithISR_strange172 (double x) const |
| double | getIntegrand_sigmaWithISR_strange183 (double x) const |
| double | getIntegrand_sigmaWithISR_strange189 (double x) const |
| double | getIntegrand_sigmaWithISR_strange192 (double x) const |
| double | getIntegrand_sigmaWithISR_strange196 (double x) const |
| double | getIntegrand_sigmaWithISR_strange200 (double x) const |
| double | getIntegrand_sigmaWithISR_strange202 (double x) const |
| double | getIntegrand_sigmaWithISR_strange205 (double x) const |
| double | getIntegrand_sigmaWithISR_strange207 (double x) const |
| double | getIntegrand_sigmaWithISR_tau130 (double x) const |
| double | getIntegrand_sigmaWithISR_tau136 (double x) const |
| double | getIntegrand_sigmaWithISR_tau161 (double x) const |
| double | getIntegrand_sigmaWithISR_tau172 (double x) const |
| double | getIntegrand_sigmaWithISR_tau183 (double x) const |
| double | getIntegrand_sigmaWithISR_tau189 (double x) const |
| double | getIntegrand_sigmaWithISR_tau192 (double x) const |
| double | getIntegrand_sigmaWithISR_tau196 (double x) const |
| double | getIntegrand_sigmaWithISR_tau200 (double x) const |
| double | getIntegrand_sigmaWithISR_tau202 (double x) const |
| double | getIntegrand_sigmaWithISR_tau205 (double x) const |
| double | getIntegrand_sigmaWithISR_tau207 (double x) const |
| double | getIntegrand_sigmaWithISR_up130 (double x) const |
| double | getIntegrand_sigmaWithISR_up133 (double x) const |
| double | getIntegrand_sigmaWithISR_up136 (double x) const |
| double | getIntegrand_sigmaWithISR_up161 (double x) const |
| double | getIntegrand_sigmaWithISR_up167 (double x) const |
| double | getIntegrand_sigmaWithISR_up172 (double x) const |
| double | getIntegrand_sigmaWithISR_up183 (double x) const |
| double | getIntegrand_sigmaWithISR_up189 (double x) const |
| double | getIntegrand_sigmaWithISR_up192 (double x) const |
| double | getIntegrand_sigmaWithISR_up196 (double x) const |
| double | getIntegrand_sigmaWithISR_up200 (double x) const |
| double | getIntegrand_sigmaWithISR_up202 (double x) const |
| double | getIntegrand_sigmaWithISR_up205 (double x) const |
| double | getIntegrand_sigmaWithISR_up207 (double x) const |
| double | Integrand_AFBnumeratorWithISR_l (double x, const QCD::lepton l_flavor, const double s) const |
| double | Integrand_AFBnumeratorWithISR_q (double x, const QCD::quark q_flavor, const double s) const |
| double | Integrand_dsigmaBox_l (double cosTheta, const QCD::lepton l_flavor, const double s) const |
| double | Integrand_dsigmaBox_q (double cosTheta, const QCD::quark q_flavor, const double s) const |
| double | Integrand_sigmaWithISR_l (double x, const QCD::lepton l_flavor, const double s) const |
| double | Integrand_sigmaWithISR_q (double x, const QCD::quark q_flavor, const double s) const |
| double | m_q (const QCD::quark q, const double mu, const orders order=FULLNLO) const |
| double | RAq (const QCD::quark q) const |
| The radiator factor associated with the final-state QED and QCD corrections to the the axial-vector-current interactions, \(R_A^q(M_Z^2)\). More... | |
| double | resumKappaZ (const double DeltaRho[orders_EW_size], const double deltaKappa_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const |
| A method to compute the real part of the effetvive coupling \(\kappa_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | resumMw (const double Mw_i, const double DeltaRho[orders_EW_size], const double DeltaR_rem[orders_EW_size]) const |
| A method to compute the \(W\)-boson mass from \(\Delta\rho\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | resumRhoZ (const double DeltaRho[orders_EW_size], const double deltaRho_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const |
| A method to compute the real part of the effective coupling \(\rho_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | RVh () const |
| The singlet vector corrections to the hadronic \(Z\)-boson width, denoted as \(R_V^h\). More... | |
| double | RVq (const QCD::quark q) const |
| The radiator factor associated with the final-state QED and QCD corrections to the the vector-current interactions, \(R_V^q(M_Z^2)\). More... | |
| double | SchemeToDouble (const std::string scheme) const |
| A method to convert a given scheme name in string form into a floating-point number with double precision. More... | |
| double | sigma_NoISR_l (const QCD::lepton l_flavor, const double s) const |
| double | sigma_NoISR_q (const QCD::quark q_flavor, const double s) const |
| double | taub () const |
| Top-mass corrections to the \(Zb\bar{b}\) vertex, denoted by \(\tau_b\). More... | |
| Protected Member Functions inherited from QCD | |
| double | MassOfNf (int nf) const |
| The Mbar mass of the heaviest quark in the theory with Nf active flavour. More... | |
Protected Attributes | |
| double | ai2G |
| double | ai3G |
| double | aiA |
| double | aiB |
| double | aiG |
| double | aiH |
| double | aiHB |
| double | aiHd |
| double | aiHe |
| double | aiHL |
| double | aiHQ |
| double | aiHu |
| double | aiHW |
| double | aipHL |
| double | aipHQ |
| double | aiT |
| double | aiu |
| double | aiuG |
| double | aiWW |
| double | aleMz |
| The em constant at Mz. More... | |
| double | BrHexo |
| The branching ratio of exotic (not invisible) Higgs decays. More... | |
| double | BrHinv |
| The branching ratio of invisible Higgs decays. More... | |
| double | C2B |
| The dimension-6 operator coefficient \(C_{2W}\). More... | |
| double | C2BS |
| The dimension-6 operator coefficient \(C_{2W}^{SILH}\). More... | |
| double | C2W |
| The dimension-6 operator coefficient \(C_{2B}\). More... | |
| double | C2WS |
| The dimension-6 operator coefficient \(C_{2B}^{SILH}\). More... | |
| double | CDB |
| The dimension-6 operator coefficient \(C_{DB}\). More... | |
| double | CdB_11i |
| The dimension-6 operator coefficient \((C_{dB})_{11}\) (imaginary part). More... | |
| double | CdB_11r |
| The dimension-6 operator coefficient \((C_{dB})_{11}\) (real part). More... | |
| double | CdB_12i |
| The dimension-6 operator coefficient \((C_{dB})_{12}\) (imaginary part). More... | |
| double | CdB_12r |
| The dimension-6 operator coefficient \((C_{dB})_{12}\) (real part). More... | |
| double | CdB_13i |
| The dimension-6 operator coefficient \((C_{dB})_{13}\) (imaginary part). More... | |
| double | CdB_13r |
| The dimension-6 operator coefficient \((C_{dB})_{13}\) (real part). More... | |
| double | CdB_22i |
| The dimension-6 operator coefficient \((C_{dB})_{22}\) (imaginary part). More... | |
| double | CdB_22r |
| The dimension-6 operator coefficient \((C_{dB})_{22}\) (real part). More... | |
| double | CdB_23i |
| The dimension-6 operator coefficient \((C_{dB})_{23}\) (imaginary part). More... | |
| double | CdB_23r |
| The dimension-6 operator coefficient \((C_{dB})_{23}\) (real part). More... | |
| double | CdB_33i |
| The dimension-6 operator coefficient \((C_{dB})_{33}\) (imaginary part). More... | |
| double | CdB_33r |
| The dimension-6 operator coefficient \((C_{dB})_{33}\) (real part). More... | |
| double | CdG_11i |
| The dimension-6 operator coefficient \((C_{dG})_{11}\) (imaginary part). More... | |
| double | CdG_11r |
| The dimension-6 operator coefficient \((C_{dG})_{11}\) (real part). More... | |
| double | CdG_12i |
| The dimension-6 operator coefficient \((C_{dG})_{12}\) (imaginary part). More... | |
| double | CdG_12r |
| The dimension-6 operator coefficient \((C_{dG})_{12}\) (real part). More... | |
| double | CdG_13i |
| The dimension-6 operator coefficient \((C_{dG})_{13}\) (imaginary part). More... | |
| double | CdG_13r |
| The dimension-6 operator coefficient \((C_{dG})_{13}\) (real part). More... | |
| double | CdG_22i |
| The dimension-6 operator coefficient \((C_{dG})_{22}\) (imaginary part). More... | |
| double | CdG_22r |
| The dimension-6 operator coefficient \((C_{dG})_{22}\) (real part). More... | |
| double | CdG_23i |
| The dimension-6 operator coefficient \((C_{dG})_{23}\) (imaginary part). More... | |
| double | CdG_23r |
| The dimension-6 operator coefficient \((C_{dG})_{23}\) (real part). More... | |
| double | CdG_33i |
| The dimension-6 operator coefficient \((C_{dG})_{33}\) (imaginary part). More... | |
| double | CdG_33r |
| The dimension-6 operator coefficient \((C_{dG})_{33}\) (real part). More... | |
| double | CdH_11i |
| The dimension-6 operator coefficient \((C_{dH})_{11}\) (imaginary part). More... | |
| double | CdH_11r |
| The dimension-6 operator coefficient \((C_{dH})_{11}\) (real part). More... | |
| double | CdH_12i |
| The dimension-6 operator coefficient \((C_{dH})_{12}\) (imaginary part). More... | |
| double | CdH_12r |
| The dimension-6 operator coefficient \((C_{dH})_{12}\) (real part). More... | |
| double | CdH_13i |
| The dimension-6 operator coefficient \((C_{dH})_{13}\) (imaginary part). More... | |
| double | CdH_13r |
| The dimension-6 operator coefficient \((C_{dH})_{13}\) (real part). More... | |
| double | CdH_22i |
| The dimension-6 operator coefficient \((C_{dH})_{22}\) (imaginary part). More... | |
| double | CdH_22r |
| The dimension-6 operator coefficient \((C_{dH})_{22}\) (real part). More... | |
| double | CdH_23i |
| The dimension-6 operator coefficient \((C_{dH})_{23}\) (imaginary part). More... | |
| double | CdH_23r |
| The dimension-6 operator coefficient \((C_{dH})_{23}\) (real part). More... | |
| double | CdH_33i |
| The dimension-6 operator coefficient \((C_{dH})_{33}\) (imaginary part). More... | |
| double | CdH_33r |
| The dimension-6 operator coefficient \((C_{dH})_{33}\) (real part). More... | |
| double | CDHB |
| The dimension-6 operator coefficient \(C_{DHB}\). More... | |
| double | CDHW |
| The dimension-6 operator coefficient \(C_{DHW}\). More... | |
| double | CDW |
| The dimension-6 operator coefficient \(C_{DW}\). More... | |
| double | CdW_11i |
| The dimension-6 operator coefficient \((C_{dW})_{11}\) (imaginary part). More... | |
| double | CdW_11r |
| The dimension-6 operator coefficient \((C_{dW})_{11}\) (real part). More... | |
| double | CdW_12i |
| The dimension-6 operator coefficient \((C_{dW})_{12}\) (imaginary part). More... | |
| double | CdW_12r |
| The dimension-6 operator coefficient \((C_{dW})_{12}\) (real part). More... | |
| double | CdW_13i |
| The dimension-6 operator coefficient \((C_{dW})_{13}\) (imaginary part). More... | |
| double | CdW_13r |
| The dimension-6 operator coefficient \((C_{dW})_{13}\) (real part). More... | |
| double | CdW_22i |
| The dimension-6 operator coefficient \((C_{dW})_{22}\) (imaginary part). More... | |
| double | CdW_22r |
| The dimension-6 operator coefficient \((C_{dW})_{22}\) (real part). More... | |
| double | CdW_23i |
| The dimension-6 operator coefficient \((C_{dW})_{23}\) (imaginary part). More... | |
| double | CdW_23r |
| The dimension-6 operator coefficient \((C_{dW})_{23}\) (real part). More... | |
| double | CdW_33i |
| The dimension-6 operator coefficient \((C_{dW})_{33}\) (imaginary part). More... | |
| double | CdW_33r |
| The dimension-6 operator coefficient \((C_{dW})_{33}\) (real part). More... | |
| double | CeB_11i |
| The dimension-6 operator coefficient \((C_{eB})_{11}\) (imaginary part). More... | |
| double | CeB_11r |
| The dimension-6 operator coefficient \((C_{eB})_{11}\) (real part). More... | |
| double | CeB_12i |
| The dimension-6 operator coefficient \((C_{eB})_{12}\) (imaginary part). More... | |
| double | CeB_12r |
| The dimension-6 operator coefficient \((C_{eB})_{12}\) (real part). More... | |
| double | CeB_13i |
| The dimension-6 operator coefficient \((C_{eB})_{13}\) (imaginary part). More... | |
| double | CeB_13r |
| The dimension-6 operator coefficient \((C_{eB})_{13}\) (real part). More... | |
| double | CeB_22i |
| The dimension-6 operator coefficient \((C_{eB})_{22}\) (imaginary part). More... | |
| double | CeB_22r |
| The dimension-6 operator coefficient \((C_{eB})_{22}\) (real part). More... | |
| double | CeB_23i |
| The dimension-6 operator coefficient \((C_{eB})_{23}\) (imaginary part). More... | |
| double | CeB_23r |
| The dimension-6 operator coefficient \((C_{eB})_{23}\) (real part). More... | |
| double | CeB_33i |
| The dimension-6 operator coefficient \((C_{eB})_{33}\) (imaginary part). More... | |
| double | CeB_33r |
| The dimension-6 operator coefficient \((C_{eB})_{33}\) (real part). More... | |
| double | Ced_1111 |
| double | Ced_1122 |
| double | Ced_1123 |
| double | Ced_1132 |
| double | Ced_1133 |
| double | Ced_2211 |
| double | Ced_2223 |
| double | Ced_2232 |
| double | Ced_3311 |
| double | Ced_3323 |
| double | Ced_3332 |
| double | Cee_1111 |
| double | Cee_1122 |
| double | Cee_1133 |
| double | Cee_2211 |
| double | Cee_3311 |
| double | CeH_11i |
| The dimension-6 operator coefficient \((C_{eH})_{11}\) (imaginary part). More... | |
| double | CeH_11r |
| The dimension-6 operator coefficient \((C_{eH})_{11}\) (real part). More... | |
| double | CeH_12i |
| The dimension-6 operator coefficient \((C_{eH})_{12}\) (imaginary part). More... | |
| double | CeH_12r |
| The dimension-6 operator coefficient \((C_{eH})_{12}\) (real part). More... | |
| double | CeH_13i |
| The dimension-6 operator coefficient \((C_{eH})_{13}\) (imaginary part). More... | |
| double | CeH_13r |
| The dimension-6 operator coefficient \((C_{eH})_{13}\) (real part). More... | |
| double | CeH_22i |
| The dimension-6 operator coefficient \((C_{eH})_{22}\) (imaginary part). More... | |
| double | CeH_22r |
| The dimension-6 operator coefficient \((C_{eH})_{22}\) (real part). More... | |
| double | CeH_23i |
| The dimension-6 operator coefficient \((C_{eH})_{23}\) (imaginary part). More... | |
| double | CeH_23r |
| The dimension-6 operator coefficient \((C_{eH})_{23}\) (real part). More... | |
| double | CeH_33i |
| The dimension-6 operator coefficient \((C_{eH})_{33}\) (imaginary part). More... | |
| double | CeH_33r |
| The dimension-6 operator coefficient \((C_{eH})_{33}\) (real part). More... | |
| double | Ceu_1111 |
| double | Ceu_1122 |
| double | Ceu_1133 |
| double | Ceu_2211 |
| double | Ceu_2233 |
| double | Ceu_3311 |
| double | CeW_11i |
| The dimension-6 operator coefficient \((C_{eW})_{11}\) (imaginary part). More... | |
| double | CeW_11r |
| The dimension-6 operator coefficient \((C_{eW})_{11}\) (real part). More... | |
| double | CeW_12i |
| The dimension-6 operator coefficient \((C_{eW})_{12}\) (imaginary part). More... | |
| double | CeW_12r |
| The dimension-6 operator coefficient \((C_{eW})_{12}\) (real part). More... | |
| double | CeW_13i |
| The dimension-6 operator coefficient \((C_{eW})_{13}\) (imaginary part). More... | |
| double | CeW_13r |
| The dimension-6 operator coefficient \((C_{eW})_{13}\) (real part). More... | |
| double | CeW_22i |
| The dimension-6 operator coefficient \((C_{eW})_{22}\) (imaginary part). More... | |
| double | CeW_22r |
| The dimension-6 operator coefficient \((C_{eW})_{22}\) (real part). More... | |
| double | CeW_23i |
| The dimension-6 operator coefficient \((C_{eW})_{23}\) (imaginary part). More... | |
| double | CeW_23r |
| The dimension-6 operator coefficient \((C_{eW})_{23}\) (real part). More... | |
| double | CeW_33i |
| The dimension-6 operator coefficient \((C_{eW})_{33}\) (imaginary part). More... | |
| double | CeW_33r |
| The dimension-6 operator coefficient \((C_{eW})_{33}\) (real part). More... | |
| double | CG |
| The dimension-6 operator coefficient \(C_{G}\). More... | |
| double | CH |
| The dimension-6 operator coefficient \(C_{H}\). More... | |
| double | CHB |
| The dimension-6 operator coefficient \(C_{HB}\). More... | |
| double | CHbox |
| The dimension-6 operator coefficient \(C_{H\Box}\). More... | |
| double | CHD |
| The dimension-6 operator coefficient \(C_{HD}\). More... | |
| double | CHd_11 |
| The dimension-6 operator coefficient \((C_{Hd})_{11}\). More... | |
| double | CHd_12i |
| The dimension-6 operator coefficient \((C_{Hd})_{12}\) (imaginary part). More... | |
| double | CHd_12r |
| The dimension-6 operator coefficient \((C_{Hd})_{12}\) (real part). More... | |
| double | CHd_13i |
| The dimension-6 operator coefficient \((C_{Hd})_{13}\) (imaginary part). More... | |
| double | CHd_13r |
| The dimension-6 operator coefficient \((C_{Hd})_{13}\) (real part). More... | |
| double | CHd_22 |
| The dimension-6 operator coefficient \((C_{Hd})_{22}\). More... | |
| double | CHd_23i |
| The dimension-6 operator coefficient \((C_{Hd})_{23}\) (imaginary part). More... | |
| double | CHd_23r |
| The dimension-6 operator coefficient \((C_{Hd})_{23}\) (real part). More... | |
| double | CHd_33 |
| The dimension-6 operator coefficient \((C_{Hd})_{33}\). More... | |
| double | CHe_11 |
| The dimension-6 operator coefficient \((C_{He})_{11}\). More... | |
| double | CHe_12i |
| The dimension-6 operator coefficient \((C_{He})_{12}\) (imaginary part). More... | |
| double | CHe_12r |
| The dimension-6 operator coefficient \((C_{He})_{12}\) (real part). More... | |
| double | CHe_13i |
| The dimension-6 operator coefficient \((C_{He})_{13}\) (imaginary part). More... | |
| double | CHe_13r |
| The dimension-6 operator coefficient \((C_{He})_{13}\) (real part). More... | |
| double | CHe_22 |
| The dimension-6 operator coefficient \((C_{He})_{22}\). More... | |
| double | CHe_23i |
| The dimension-6 operator coefficient \((C_{He})_{23}\) (imaginary part). More... | |
| double | CHe_23r |
| The dimension-6 operator coefficient \((C_{He})_{23}\) (real part). More... | |
| double | CHe_33 |
| The dimension-6 operator coefficient \((C_{He})_{33}\). More... | |
| double | CHG |
| The dimension-6 operator coefficient \(C_{HG}\). More... | |
| double | CHL1_11 |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\). More... | |
| double | CHL1_12i |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part). More... | |
| double | CHL1_12r |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part). More... | |
| double | CHL1_13i |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part). More... | |
| double | CHL1_13r |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part). More... | |
| double | CHL1_22 |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\). More... | |
| double | CHL1_23i |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part). More... | |
| double | CHL1_23r |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part). More... | |
| double | CHL1_33 |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\). More... | |
| double | CHL3_11 |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\). More... | |
| double | CHL3_12i |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More... | |
| double | CHL3_12r |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More... | |
| double | CHL3_13i |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More... | |
| double | CHL3_13r |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More... | |
| double | CHL3_22 |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\). More... | |
| double | CHL3_23i |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More... | |
| double | CHL3_23r |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More... | |
| double | CHL3_33 |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\). More... | |
| double | CHQ1_11 |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\). More... | |
| double | CHQ1_12i |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part). More... | |
| double | CHQ1_12r |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part). More... | |
| double | CHQ1_13i |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part). More... | |
| double | CHQ1_13r |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part). More... | |
| double | CHQ1_22 |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\). More... | |
| double | CHQ1_23i |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part). More... | |
| double | CHQ1_23r |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part). More... | |
| double | CHQ1_33 |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\). More... | |
| double | CHQ3_11 |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\). More... | |
| double | CHQ3_12i |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part). More... | |
| double | CHQ3_12r |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part). More... | |
| double | CHQ3_13i |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part). More... | |
| double | CHQ3_13r |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part). More... | |
| double | CHQ3_22 |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\). More... | |
| double | CHQ3_23i |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part). More... | |
| double | CHQ3_23r |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part). More... | |
| double | CHQ3_33 |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\). More... | |
| double | cHSM |
| Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes. More... | |
| double | CHu_11 |
| The dimension-6 operator coefficient \((C_{Hu})_{11}\). More... | |
| double | CHu_12i |
| The dimension-6 operator coefficient \((C_{Hu})_{12}\) (imaginary part). More... | |
| double | CHu_12r |
| The dimension-6 operator coefficient \((C_{Hu})_{12}\) (real part). More... | |
| double | CHu_13i |
| The dimension-6 operator coefficient \((C_{Hu})_{13}\) (imaginary part). More... | |
| double | CHu_13r |
| The dimension-6 operator coefficient \((C_{Hu})_{13}\) (real part). More... | |
| double | CHu_22 |
| The dimension-6 operator coefficient \((C_{Hu})_{22}\). More... | |
| double | CHu_23i |
| The dimension-6 operator coefficient \((C_{Hu})_{23}\) (imaginary part). More... | |
| double | CHu_23r |
| The dimension-6 operator coefficient \((C_{Hu})_{23}\) (real part). More... | |
| double | CHu_33 |
| The dimension-6 operator coefficient \((C_{Hu})_{33}\). More... | |
| double | CHud_11i |
| The dimension-6 operator coefficient \((C_{Hud})_{11}\) (imaginary part). More... | |
| double | CHud_11r |
| The dimension-6 operator coefficient \((C_{Hud})_{11}\) (real part). More... | |
| double | CHud_12i |
| The dimension-6 operator coefficient \((C_{Hud})_{12}\) (imaginary part). More... | |
| double | CHud_12r |
| The dimension-6 operator coefficient \((C_{Hud})_{12}\) (real part). More... | |
| double | CHud_13i |
| The dimension-6 operator coefficient \((C_{Hud})_{13}\) (imaginary part). More... | |
| double | CHud_13r |
| The dimension-6 operator coefficient \((C_{Hud})_{13}\) (real part). More... | |
| double | CHud_22i |
| The dimension-6 operator coefficient \((C_{Hud})_{22}\) (imaginary part). More... | |
| double | CHud_22r |
| The dimension-6 operator coefficient \((C_{Hud})_{22}\) (real part). More... | |
| double | CHud_23i |
| The dimension-6 operator coefficient \((C_{Hud})_{23}\) (imaginary part). More... | |
| double | CHud_23r |
| The dimension-6 operator coefficient \((C_{Hud})_{23}\) (real part). More... | |
| double | CHud_33i |
| The dimension-6 operator coefficient \((C_{Hud})_{33}\) (imaginary part). More... | |
| double | CHud_33r |
| The dimension-6 operator coefficient \((C_{Hud})_{33}\) (real part). More... | |
| double | CHW |
| The dimension-6 operator coefficient \(C_{HW}\). More... | |
| double | CHWB |
| The dimension-6 operator coefficient \(C_{HWB}\). More... | |
| double | CHWHB_gaga |
| The combination of dimension-6 operator coefficients entering in \(\delta_{AA}\): \(s_W^2 C_{HW} + c_W^2 C_{HW}\). More... | |
| double | CHWHB_gagaorth |
| The combination of dimension-6 operator coefficients \(-c_W^2 C_{HW} + s_W^2 C_{HW}\). More... | |
| double | CidH_11r |
| double | CidH_22r |
| double | CidH_33r |
| double | CiDHB |
| double | CiDHW |
| double | CieH_11r |
| double | CieH_22r |
| double | CieH_33r |
| double | CiH |
| double | CiHB |
| double | CiHbox |
| double | CiHD |
| double | CiHd_11 |
| double | CiHd_22 |
| double | CiHd_33 |
| double | CiHe_11 |
| double | CiHe_22 |
| double | CiHe_33 |
| double | CiHL1_11 |
| double | CiHL1_22 |
| double | CiHL1_33 |
| double | CiHL3_11 |
| double | CiHL3_22 |
| double | CiHL3_33 |
| double | CiHQ1_11 |
| double | CiHQ1_22 |
| double | CiHQ1_33 |
| double | CiHQ3_11 |
| double | CiHQ3_22 |
| double | CiHQ3_33 |
| double | CiHu_11 |
| double | CiHu_22 |
| double | CiHu_33 |
| double | CiHW |
| double | CiHWB |
| double | CiLL_1221 |
| double | CiLL_2112 |
| double | CiuB_11r |
| double | CiuB_22r |
| double | CiuB_33r |
| double | CiuG_11r |
| double | CiuG_22r |
| double | CiuG_33r |
| double | CiuH_11r |
| double | CiuH_22r |
| double | CiuH_33r |
| double | CiuW_11r |
| double | CiuW_22r |
| double | CiuW_33r |
| double | CiW |
| double | CLd_1111 |
| double | CLd_1122 |
| double | CLd_1123 |
| double | CLd_1132 |
| double | CLd_1133 |
| double | CLd_2211 |
| double | CLd_2223 |
| double | CLd_2232 |
| double | CLd_3311 |
| double | CLd_3323 |
| double | CLd_3332 |
| double | CLe_1111 |
| double | CLe_1122 |
| double | CLe_1133 |
| double | CLe_2211 |
| double | CLe_3311 |
| double | CLedQ_11 |
| double | CLedQ_22 |
| double | cLH3d62 |
| Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions modifying the Higgs trilinear coupling (Quadratic terms). More... | |
| double | cLHd6 |
| Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions. More... | |
| double | CLL_1111 |
| double | CLL_1122 |
| double | CLL_1133 |
| double | CLL_1221 |
| double | CLL_1331 |
| double | CLL_2112 |
| double | CLL_2211 |
| double | CLL_3113 |
| double | CLL_3311 |
| double | CLQ1_1111 |
| double | CLQ1_1122 |
| double | CLQ1_1123 |
| double | CLQ1_1132 |
| double | CLQ1_1133 |
| double | CLQ1_1221 |
| double | CLQ1_1331 |
| double | CLQ1_2112 |
| double | CLQ1_2211 |
| double | CLQ1_2223 |
| double | CLQ1_2232 |
| double | CLQ1_3113 |
| double | CLQ1_3311 |
| double | CLQ1_3323 |
| double | CLQ1_3332 |
| double | CLQ3_1111 |
| double | CLQ3_1122 |
| double | CLQ3_1123 |
| double | CLQ3_1132 |
| double | CLQ3_1133 |
| double | CLQ3_1221 |
| double | CLQ3_1331 |
| double | CLQ3_2112 |
| double | CLQ3_2211 |
| double | CLQ3_2223 |
| double | CLQ3_2232 |
| double | CLQ3_3113 |
| double | CLQ3_3311 |
| double | CLQ3_3323 |
| double | CLQ3_3332 |
| double | CLu_1111 |
| double | CLu_1122 |
| double | CLu_1133 |
| double | CLu_2211 |
| double | CLu_2233 |
| double | CLu_3311 |
| double | CpLedQ_11 |
| double | CpLedQ_22 |
| double | CQe_1111 |
| double | CQe_1122 |
| double | CQe_1133 |
| double | CQe_2211 |
| double | CQe_2311 |
| double | CQe_2322 |
| double | CQe_2333 |
| double | CQe_3211 |
| double | CQe_3222 |
| double | CQe_3233 |
| double | CQe_3311 |
| double | CT |
| The dimension-6 operator coefficient \(C_{T}\). More... | |
| double | CuB_11i |
| The dimension-6 operator coefficient \((C_{uB})_{11}\) (imaginary part). More... | |
| double | CuB_11r |
| The dimension-6 operator coefficient \((C_{uB})_{11}\) (real part). More... | |
| double | CuB_12i |
| The dimension-6 operator coefficient \((C_{uB})_{12}\) (imaginary part). More... | |
| double | CuB_12r |
| The dimension-6 operator coefficient \((C_{uB})_{12}\) (real part). More... | |
| double | CuB_13i |
| The dimension-6 operator coefficient \((C_{uB})_{13}\) (imaginary part). More... | |
| double | CuB_13r |
| The dimension-6 operator coefficient \((C_{uB})_{13}\) (real part). More... | |
| double | CuB_22i |
| The dimension-6 operator coefficient \((C_{uB})_{22}\) (imaginary part). More... | |
| double | CuB_22r |
| The dimension-6 operator coefficient \((C_{uB})_{22}\) (real part). More... | |
| double | CuB_23i |
| The dimension-6 operator coefficient \((C_{uB})_{23}\) (imaginary part). More... | |
| double | CuB_23r |
| The dimension-6 operator coefficient \((C_{uB})_{23}\) (real part). More... | |
| double | CuB_33i |
| The dimension-6 operator coefficient \((C_{uB})_{33}\) (imaginary part). More... | |
| double | CuB_33r |
| The dimension-6 operator coefficient \((C_{uB})_{33}\) (real part). More... | |
| double | CuG_11i |
| The dimension-6 operator coefficient \((C_{uG})_{11}\) (imaginary part). More... | |
| double | CuG_11r |
| The dimension-6 operator coefficient \((C_{uG})_{11}\) (real part). More... | |
| double | CuG_12i |
| The dimension-6 operator coefficient \((C_{uG})_{12}\) (imaginary part). More... | |
| double | CuG_12r |
| The dimension-6 operator coefficient \((C_{uG})_{12}\) (real part). More... | |
| double | CuG_13i |
| The dimension-6 operator coefficient \((C_{uG})_{13}\) (imaginary part). More... | |
| double | CuG_13r |
| The dimension-6 operator coefficient \((C_{uG})_{13}\) (real part). More... | |
| double | CuG_22i |
| The dimension-6 operator coefficient \((C_{uG})_{22}\) (imaginary part). More... | |
| double | CuG_22r |
| The dimension-6 operator coefficient \((C_{uG})_{22}\) (real part). More... | |
| double | CuG_23i |
| The dimension-6 operator coefficient \((C_{uG})_{23}\) (imaginary part). More... | |
| double | CuG_23r |
| The dimension-6 operator coefficient \((C_{uG})_{23}\) (real part). More... | |
| double | CuG_33i |
| The dimension-6 operator coefficient \((C_{uG})_{33}\) (imaginary part). More... | |
| double | CuG_33r |
| The dimension-6 operator coefficient \((C_{uG})_{33}\) (real part). More... | |
| double | CuH_11i |
| The dimension-6 operator coefficient \((C_{uH})_{11}\) (imaginary part). More... | |
| double | CuH_11r |
| The dimension-6 operator coefficient \((C_{uH})_{11}\) (real part). More... | |
| double | CuH_12i |
| The dimension-6 operator coefficient \((C_{uH})_{12}\) (imaginary part). More... | |
| double | CuH_12r |
| The dimension-6 operator coefficient \((C_{uH})_{12}\) (real part). More... | |
| double | CuH_13i |
| The dimension-6 operator coefficient \((C_{uH})_{13}\) (imaginary part). More... | |
| double | CuH_13r |
| The dimension-6 operator coefficient \((C_{uH})_{13}\) (real part). More... | |
| double | CuH_22i |
| The dimension-6 operator coefficient \((C_{uH})_{22}\) (imaginary part). More... | |
| double | CuH_22r |
| The dimension-6 operator coefficient \((C_{uH})_{22}\) (real part). More... | |
| double | CuH_23i |
| The dimension-6 operator coefficient \((C_{uH})_{23}\) (imaginary part). More... | |
| double | CuH_23r |
| The dimension-6 operator coefficient \((C_{uH})_{23}\) (real part). More... | |
| double | CuH_33i |
| The dimension-6 operator coefficient \((C_{uH})_{33}\) (imaginary part). More... | |
| double | CuH_33r |
| The dimension-6 operator coefficient \((C_{uH})_{33}\) (real part). More... | |
| double | CuW_11i |
| The dimension-6 operator coefficient \((C_{uW})_{11}\) (imaginary part). More... | |
| double | CuW_11r |
| The dimension-6 operator coefficient \((C_{uW})_{11}\) (real part). More... | |
| double | CuW_12i |
| The dimension-6 operator coefficient \((C_{uW})_{12}\) (imaginary part). More... | |
| double | CuW_12r |
| The dimension-6 operator coefficient \((C_{uW})_{12}\) (real part). More... | |
| double | CuW_13i |
| The dimension-6 operator coefficient \((C_{uW})_{13}\) (imaginary part). More... | |
| double | CuW_13r |
| The dimension-6 operator coefficient \((C_{uW})_{13}\) (real part). More... | |
| double | CuW_22i |
| The dimension-6 operator coefficient \((C_{uW})_{22}\) (imaginary part). More... | |
| double | CuW_22r |
| The dimension-6 operator coefficient \((C_{uW})_{22}\) (real part). More... | |
| double | CuW_23i |
| The dimension-6 operator coefficient \((C_{uW})_{23}\) (imaginary part). More... | |
| double | CuW_23r |
| The dimension-6 operator coefficient \((C_{uW})_{23}\) (real part). More... | |
| double | CuW_33i |
| The dimension-6 operator coefficient \((C_{uW})_{33}\) (imaginary part). More... | |
| double | CuW_33r |
| The dimension-6 operator coefficient \((C_{uW})_{33}\) (real part). More... | |
| double | CW |
| The dimension-6 operator coefficient \(C_{W}\). More... | |
| double | cW2_tree |
| The square of the tree level values for the cosine of the weak angle. More... | |
| double | cW_tree |
| The tree level values for the cosine of the weak angle. More... | |
| double | delta_AA |
| Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More... | |
| double | delta_AZ |
| Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More... | |
| double | delta_h |
| Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition. More... | |
| double | delta_ZZ |
| Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition. More... | |
| double | dg1Z |
| Independent contribution to aTGC. More... | |
| double | dGammaHTotR1 |
| double | dGammaHTotR2 |
| double | dKappaga |
| Independent contribution to aTGC. More... | |
| double | dZH |
| Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization. More... | |
| double | eeettHint |
| Intrinsic relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More... | |
| double | eeettHpar |
| Parametric relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More... | |
| double | eeeWBFint |
| Intrinsic relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More... | |
| double | eeeWBFpar |
| Parametric relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More... | |
| double | eeeZHint |
| Intrinsic relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More... | |
| double | eeeZHpar |
| Parametric relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More... | |
| double | eeMz |
| The em coupling at Mz. More... | |
| double | eeMz2 |
| The em coupling squared (at Mz). More... | |
| double | eepWBFint |
| Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.) More... | |
| double | eepWBFpar |
| Parametric relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.) More... | |
| double | eepZBFint |
| Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.) More... | |
| double | eepZBFpar |
| Parametric relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.) More... | |
| double | eggFHbb |
| double | eggFHgaga |
| double | eggFHmumu |
| Total relative theoretical error in \(gg \to H \to X\). More... | |
| double | eggFHtautau |
| double | eggFHWW |
| double | eggFHZga |
| double | eggFHZZ |
| double | eggFint |
| Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.) More... | |
| double | eggFpar |
| Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.) More... | |
| double | eHbbint |
| Intrinsic relative theoretical error in \(H \to b\bar{b}\). More... | |
| double | eHbbpar |
| Parametric relative theoretical error in \(H \to b\bar{b}\). More... | |
| double | eHccint |
| Intrinsic relative theoretical error in \(H \to c\bar{c}\). More... | |
| double | eHccpar |
| Parametric relative theoretical error in \(H \to c\bar{c}\). More... | |
| double | eHgagaint |
| Intrinsic relative theoretical error in \(H \to \gamma\gamma\). More... | |
| double | eHgagapar |
| Parametric relative theoretical error in \(H \to \gamma\gamma\). More... | |
| double | eHggint |
| Intrinsic relative theoretical error in \(H \to g g\). More... | |
| double | eHggpar |
| Parametric relative theoretical error in \(H \to g g\). More... | |
| double | eHmumuint |
| Intrinsic relative theoretical error in \(H \to \mu^+ \mu^-\). More... | |
| double | eHmumupar |
| Parametric relative theoretical error in \(H \to \mu^+ \mu^-\). More... | |
| double | eHtautauint |
| Intrinsic relative theoretical error in \(H \to \tau^+ \tau^-\). More... | |
| double | eHtautaupar |
| Parametric relative theoretical error in \(H \to \tau^+ \tau^-\). More... | |
| double | eHwidth |
| Total relative theoretical error in the Higgs width. More... | |
| double | eHWWint |
| Intrinsic relative theoretical error in \(H \to W W\). More... | |
| double | eHWWpar |
| Parametric relative theoretical error in \(H \to W W\). More... | |
| double | eHZgaint |
| Intrinsic relative theoretical error in \(H \to Z \gamma\). More... | |
| double | eHZgapar |
| Parametric relative theoretical error in \(H \to Z \gamma\). More... | |
| double | eHZZint |
| Intrinsic relative theoretical error in \(H \to Z Z\). More... | |
| double | eHZZpar |
| Parametric relative theoretical error in \(H \to Z Z\). More... | |
| double | ettH_1314_DeltagHt |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (13 & 14 TeV). More... | |
| double | ettH_1314_G |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (13 & 14 TeV). More... | |
| double | ettH_1314_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (13 & 14 TeV). More... | |
| double | ettH_1314_uG_33r |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (13 & 14 TeV). More... | |
| double | ettH_2_DeltagHt |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (1.96 TeV). More... | |
| double | ettH_2_G |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (1.96 TeV). More... | |
| double | ettH_2_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (1.96 TeV). More... | |
| double | ettH_2_uG_33r |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (1.96 TeV). More... | |
| double | ettH_78_DeltagHt |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (7 & 8 TeV). More... | |
| double | ettH_78_G |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (7 & 8 TeV). More... | |
| double | ettH_78_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (7 & 8 TeV). More... | |
| double | ettH_78_uG_33r |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (7 & 8 TeV). More... | |
| double | ettHbb |
| double | ettHgaga |
| double | ettHint |
| Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.) More... | |
| double | ettHmumu |
| Total relative theoretical error in \(pp \to ttH \to tt X\). More... | |
| double | ettHpar |
| Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.) More... | |
| double | ettHtautau |
| double | ettHWW |
| double | ettHZga |
| double | ettHZZ |
| double | eVBF_1314_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_2_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_78_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBFHbb |
| double | eVBFHgaga |
| double | eVBFHinv |
| double | eVBFHmumu |
| Total relative theoretical error in \(pp \to Hjj (VBF) \to X jj\). More... | |
| double | eVBFHtautau |
| double | eVBFHWW |
| double | eVBFHZga |
| double | eVBFHZZ |
| double | eVBFint |
| Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.) More... | |
| double | eVBFpar |
| Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.) More... | |
| double | eVHinv |
| Total relative theoretical error in \(pp \to X H \to X + invisible\). More... | |
| double | eWH_1314_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (13 & 14 TeV). More... | |
| double | eWH_1314_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (13 & 14 TeV). More... | |
| double | eWH_1314_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (13 & 14 TeV). More... | |
| double | eWH_1314_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (13 & 14 TeV). More... | |
| double | eWH_1314_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (13 & 14 TeV). More... | |
| double | eWH_1314_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (13 & 14 TeV). More... | |
| double | eWH_1314_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (13 & 14 TeV). More... | |
| double | eWH_2_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (1.96 TeV). More... | |
| double | eWH_2_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (1.96 TeV). More... | |
| double | eWH_2_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH_2_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH_2_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH_2_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH_2_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH_78_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (7 & 8 TeV). More... | |
| double | eWH_78_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (7 & 8 TeV). More... | |
| double | eWH_78_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (7 & 8 TeV). More... | |
| double | eWH_78_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (7 & 8 TeV). More... | |
| double | eWH_78_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (7 & 8 TeV). More... | |
| double | eWH_78_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (7 & 8 TeV). More... | |
| double | eWH_78_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (7 & 8 TeV). More... | |
| double | eWHbb |
| double | eWHgaga |
| double | eWHint |
| Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.) More... | |
| double | eWHmumu |
| Total relative theoretical error in \(pp \to WH \to W X\). More... | |
| double | eWHpar |
| Parametric relative theoretical error in WH production. (Assumed to be constant in energy.) More... | |
| double | eWHtautau |
| double | eWHWW |
| double | eWHZga |
| double | eWHZZ |
| double | eZH_1314_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_2_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_78_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZHbb |
| double | eZHgaga |
| double | eZHint |
| Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.) More... | |
| double | eZHmumu |
| Total relative theoretical error in \(pp \to ZH \to Z X\). More... | |
| double | eZHpar |
| Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.) More... | |
| double | eZHtautau |
| double | eZHWW |
| double | eZHZga |
| double | eZHZZ |
| double | g1_tree |
| The tree level value of the \(U(1)_Y\) gauge coupling contant (at the \(Z\) pole). More... | |
| double | g2_tree |
| The tree level value of the \(SU(2)_L\) gauge coupling contant (at the \(Z\) pole). More... | |
| double | g3_tree |
| The tree level value of the \(SU(3)_c\) gauge coupling contant (at the \(Z\) pole). More... | |
| double | GammaHTotR |
| NP contributions and Total to Higgs width ratio with SM. More... | |
| double | gZdL |
| double | gZdR |
| The tree level value of the \(Z\bar{d}d\) couplings in the SM. More... | |
| double | gZlL |
| double | gZlR |
| The tree level value of the \(Z\ell^+\ell^-\) couplings in the SM. More... | |
| double | gZuL |
| double | gZuR |
| The tree level value of the \(Z\bar{u}u\) couplings in the SM. More... | |
| double | gZvL |
| The tree level value of the \(Z\bar{\nu}\nu\) couplings in the SM. More... | |
| double | Lambda_NP |
| The new physics scale [GeV]. More... | |
| double | lambdaH_tree |
| The SM tree level value of the scalar quartic coupling in the potential. More... | |
| double | LambdaNP2 |
| The square of the new physics scale [GeV \(^2\)]. More... | |
| double | lambZ |
| Independent contribution to aTGC. More... | |
| Matching< NPSMEFTd6Matching, NPSMEFTd6 > | NPSMEFTd6M |
| double | sW2_tree |
| The square of the tree level values for the sine of the weak angle. More... | |
| double | sW_tree |
| The tree level values for the sine of the weak angle. More... | |
| double | UevL |
| The tree level value of the \(W^-\bar{\ell}\nu\) couplings in the SM. (Neglecting PMNS effects.) More... | |
| double | v2 |
| The square of the EW vev. More... | |
| double | v2_over_LambdaNP2 |
| The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\). More... | |
| double | VudL |
| The tree level value of the \(W^+\bar{u}d\) couplings in the SM. (Neglecting CKM effects.) More... | |
| double | Yukb |
| SM d-quark Yukawas. More... | |
| double | Yukc |
| double | Yukd |
| double | Yuke |
| double | Yukmu |
| double | Yuks |
| double | Yukt |
| SM u-quark Yukawas. More... | |
| double | Yuktau |
| SM lepton Yukawas. More... | |
| double | Yuku |
| Protected Attributes inherited from NPbase | |
| StandardModel | trueSM |
| Protected Attributes inherited from StandardModel | |
| double | A |
| The CKM parameter \(A\) in the Wolfenstein parameterization. More... | |
| double | ale |
| The fine-structure constant \(\alpha\). More... | |
| double | alpha21 |
| double | alpha31 |
| double | AlsMz |
| The strong coupling constant at the Z-boson mass, \(\alpha_s(M_Z)\). More... | |
| bool | bSigmaForAFB |
| bool | bSigmaForR |
| double | dAle5Mz |
| The five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More... | |
| double | delGammaZ |
| The theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\), in GeV. More... | |
| double | delMw |
| The theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\), in GeV. More... | |
| double | delR0b |
| The theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More... | |
| double | delR0c |
| The theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More... | |
| double | delR0l |
| The theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More... | |
| double | delsigma0H |
| The theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\) in nb. More... | |
| double | delSin2th_b |
| The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More... | |
| double | delSin2th_l |
| The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More... | |
| double | delSin2th_q |
| The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More... | |
| double | delta |
| double | etab |
| The CKM parameter \(\bar{\eta}\) in the Wolfenstein parameterization. More... | |
| bool | flag_order [orders_EW_size] |
| An array of internal flags controlling the inclusions of higher-order corrections. More... | |
| bool | flagLEP2 [NUMofLEP2RCs] |
| double | gamma |
| \(\gamma \) used as an input for FlagWolfenstein = FALSE More... | |
| double | GF |
| The Fermi constant \(G_\mu\) in \({\rm GeV}^{-2}\). More... | |
| double | lambda |
| The CKM parameter \(\lambda\) in the Wolfenstein parameterization. More... | |
| Particle | leptons [6] |
| An array of Particle objects for the leptons. More... | |
| double | mHl |
| The Higgs mass \(m_h\) in GeV. More... | |
| double | muw |
| A matching scale \(\mu_W\) around the weak scale in GeV. More... | |
| CKM | myCKM |
| An object of type CKM. More... | |
| PMNS | myPMNS |
| double | Mz |
| The mass of the \(Z\) boson in GeV. More... | |
| bool | requireCKM |
| An internal flag to control whether the CKM matrix has to be recomputed. More... | |
| bool | requireYe |
| An internal flag to control whether the charged-lepton Yukawa matrix has to be recomputed. More... | |
| bool | requireYn |
| An internal flag to control whether the neutrino Yukawa matrix has to be recomputed. More... | |
| double | rhob |
| The CKM parameter \(\bar{\rho}\) in the Wolfenstein parameterization. More... | |
| double | s12 |
| double | s13 |
| double | s23 |
| Flavour | SMFlavour |
| An object of type Flavour. More... | |
| Matching< StandardModelMatching, StandardModel > | SMM |
| An object of type Matching. More... | |
| double | Vcb |
| \(\vert V_{cb} \vert \) used as an input for FlagWolfenstein = FALSE More... | |
| double | Vub |
| \(\vert V_{ub} \vert \) used as an input for FlagWolfenstein = FALSE More... | |
| double | Vus |
| \(\vert V_{us} \vert \) used as an input for FlagWolfenstein = FALSE More... | |
| gslpp::matrix< gslpp::complex > | Yd |
| The Yukawa matrix of the down-type quarks. More... | |
| gslpp::matrix< gslpp::complex > | Ye |
| The Yukawa matrix of the charged leptons. More... | |
| gslpp::matrix< gslpp::complex > | Yn |
| The Yukawa matrix of the neutrinos. More... | |
| gslpp::matrix< gslpp::complex > | Yu |
| The Yukawa matrix of the up-type quarks. More... | |
| Protected Attributes inherited from QCD | |
| double | AlsM |
| The strong coupling constant at the mass scale MAls, \(\alpha_s(M_{\alpha_s})\). More... | |
| double | CA |
| double | CF |
| bool | computemt |
| Switch for computing the \(\overline{\mathrm{MS}}\) mass of the top quark. More... | |
| double | dAdA_NA |
| double | dFdA_NA |
| double | dFdF_NA |
| double | MAls |
| The mass scale in GeV at which the strong coupling measurement is provided. More... | |
| double | mtpole |
| The pole mass of the top quark. More... | |
| double | mub |
| The threshold between five- and four-flavour theory in GeV. More... | |
| double | muc |
| The threshold between four- and three-flavour theory in GeV. More... | |
| double | mut |
| The threshold between six- and five-flavour theory in GeV. More... | |
| double | NA |
| double | Nc |
| The number of colours. More... | |
| Particle | quarks [6] |
| The vector of all SM quarks. More... | |
| bool | requireYd |
| Switch for generating the Yukawa couplings to the down-type quarks. More... | |
| bool | requireYu |
| Switch for generating the Yukawa couplings to the up-type quarks. More... | |
| double | TF |
| Protected Attributes inherited from Model | |
| bool | isSliced |
| A boolean set to true if the current istance is a slice of an extended object. More... | |
| std::map< std::string, std::reference_wrapper< const double > > | ModelParamMap |
| bool | UpdateError |
| A boolean set to false if update is successful. More... | |
Private Attributes | |
| bool | FlagFlavU3OfX |
| A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients. More... | |
| bool | FlagHiggsSM |
| A boolean flag that is true if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables. More... | |
| const bool | FlagLeptonUniversal |
| An internal boolean flag that is true if assuming lepton flavour universality. More... | |
| bool | FlagLoopH3d6Quad |
| A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling. More... | |
| bool | FlagLoopHd6 |
| A boolean flag that is true if including modifications in the SM loops in Higgs observables due to the dim 6 interactions. More... | |
| bool | FlagPartialQFU |
| A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd family in the CHF operators. More... | |
| bool | FlagQuadraticTerms |
| A boolean flag that is true if the quadratic terms in cross sections and widths are switched on. More... | |
| const bool | FlagQuarkUniversal |
| An internal boolean flag that is true if assuming quark flavour universality. More... | |
| bool | FlagRotateCHWCHB |
| A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and CHB. More... | |
| bool | FlagUnivOfX |
| A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and all proportional to the same coefficient (CuH_33 and CuV_33 respectively). More... | |
| gsl_integration_cquad_workspace * | w_WW |
Additional Inherited Members | |
| Public Types inherited from StandardModel | |
| enum | LEP2RCs { Weak = 0, WeakBox, ISR, QEDFSR, QCDFSR, NUMofLEP2RCs } |
| enum | orders_EW { EW1 = 0, EW1QCD1, EW1QCD2, EW2, EW2QCD1, EW3, orders_EW_size } |
| An enumerated type representing perturbative orders of radiative corrections to EW precision observables. More... | |
| Public Types inherited from QCD | |
| enum | lepton { NEUTRINO_1, ELECTRON, NEUTRINO_2, MU, NEUTRINO_3, TAU, NOLEPTON } |
| An enum type for leptons. More... | |
| enum | meson { P_0, P_P, K_0, K_P, D_0, D_P, B_D, B_P, B_S, B_C, PHI, K_star, K_star_P, D_star_P, RHO, RHO_P, OMEGA, MESON_END } |
| An enum type for mesons. More... | |
| enum | quark { UP, DOWN, CHARM, STRANGE, TOP, BOTTOM } |
| An enum type for quarks. More... | |
| NPSMEFTd6::NPSMEFTd6 | ( | const bool | FlagLeptonUniversal_in = false, |
| const bool | FlagQuarkUniversal_in = false |
||
| ) |
Constructor.
| [in] | FlagLeptonUniversal_in | an internal boolean flag that is true if assuming lepton flavour universality |
| [in] | FlagQuarkUniversal_in | an internal boolean flag that is true if assuming quark flavour universality |
Definition at line 304 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::AH_f | ( | const double | tau | ) | const |
Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.
\(A^H_f(\tau)=2\tau [1+(1-\tau)f(\tau)]\)
| [in] |
Definition at line 3595 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::AH_W | ( | const double | tau | ) | const |
W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling.
\(A^H_W(\tau)=-[2+3\tau + 3\tau*(2-\tau) f(\tau)]\)
| [in] |
Definition at line 3600 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::AHZga_f | ( | const double | tau, |
| const double | lambda | ||
| ) | const |
Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling.
| [in] |
Definition at line 3605 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::AHZga_W | ( | const double | tau, |
| const double | lambda | ||
| ) | const |
W loop function entering in the calculation of the effective \(HZ\gamma\) coupling.
| [in] |
Definition at line 3610 of file NPSMEFTd6.cpp.
|
virtual |
the angular parameter \(a\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]).
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 8939 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP1 (See code for details.)
Reimplemented from NPbase.
Definition at line 15619 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP10 (See code for details.)
Reimplemented from NPbase.
Definition at line 16220 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP11 (See code for details.)
Reimplemented from NPbase.
Definition at line 16251 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP12 (See code for details.)
Reimplemented from NPbase.
Definition at line 16282 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP13.
Reimplemented from NPbase.
Definition at line 16298 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP14.
Reimplemented from NPbase.
Definition at line 16314 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP15.
Reimplemented from NPbase.
Definition at line 16426 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP16.
Reimplemented from NPbase.
Definition at line 16432 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP17.
Reimplemented from NPbase.
Definition at line 16438 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP18.
Reimplemented from NPbase.
Definition at line 16444 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP19.
Reimplemented from NPbase.
Definition at line 16450 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP2 (See code for details.)
Reimplemented from NPbase.
Definition at line 15646 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP20.
Reimplemented from NPbase.
Definition at line 16456 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP3 (See code for details.)
Reimplemented from NPbase.
Definition at line 15674 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP4 (See code for details.)
Reimplemented from NPbase.
Definition at line 15702 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP5 (See code for details.)
Reimplemented from NPbase.
Definition at line 15766 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP6 (See code for details.)
Reimplemented from NPbase.
Definition at line 15837 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP7 (See code for details.)
Reimplemented from NPbase.
Definition at line 16105 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP8 (See code for details.)
Reimplemented from NPbase.
Definition at line 16138 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP9 (See code for details.)
Reimplemented from NPbase.
Definition at line 16158 of file NPSMEFTd6.cpp.
|
virtual |
the angular parameter \(b\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]).
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 9022 of file NPSMEFTd6.cpp.
|
virtual |
The branching ratio of the of the Higgs into exotic particles.
Reimplemented from NPbase.
Definition at line 12713 of file NPSMEFTd6.cpp.
|
virtual |
The branching ratio of the of the Higgs into invisible particles.
Reimplemented from NPbase.
Definition at line 12720 of file NPSMEFTd6.cpp.
|
virtual |
The branching ratio of the of the Higgs into invisible particles (only invisible new particles).
Reimplemented from NPbase.
Definition at line 12735 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10866 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10840 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10762 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10202 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10788 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10814 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 12794 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 12746 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 10335 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to W j j)\) in the current model and in the Standard Model.
Definition at line 10285 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10235 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10260 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 10361 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to WW^*\to 4j)\) in the current model and in the Standard Model.
Definition at line 10310 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10228 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.
Definition at line 10606 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 10649 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10740 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10725 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10751 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10699 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10391 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model.
Definition at line 10566 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z\nu\nu)\) in the current model and in the Standard Model.
Definition at line 10516 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10466 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.
Definition at line 10631 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10441 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 10674 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10416 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10491 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model.
Definition at line 10591 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model.
Definition at line 10541 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10386 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 2893 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 2841 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 2815 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 2867 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 15570 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 15580 of file NPSMEFTd6.cpp.
|
virtual |
The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 15589 of file NPSMEFTd6.cpp.
|
virtual |
A method to check if all the mandatory parameters for NPSMEFTd6 have been provided in model initialization.
| [in] | DPars | a map of the parameters that are being updated in the Monte Carlo run (including parameters that are varied and those that are held constant) |
Reimplemented from StandardModel.
Definition at line 2652 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F.
| [in] | F | a lepton or quark |
Definition at line 2738 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F.
| [in] | F | a lepton or quark |
Definition at line 2756 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 2774 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{Hud}\) corresponding to particle f.
| [in] | u | a quark |
Definition at line 2800 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLL_bottom | ( | ) | const |
| double NPSMEFTd6::CLL_charm | ( | ) | const |
| double NPSMEFTd6::CLL_down | ( | ) | const |
Definition at line 16479 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLL_mu | ( | ) | const |
| double NPSMEFTd6::CLL_strange | ( | ) | const |
| double NPSMEFTd6::CLL_tau | ( | ) | const |
| double NPSMEFTd6::CLL_up | ( | ) | const |
Definition at line 16474 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLR_bottom | ( | ) | const |
Definition at line 16529 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLR_charm | ( | ) | const |
Definition at line 16519 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLR_down | ( | ) | const |
Definition at line 16514 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLR_mu | ( | ) | const |
Definition at line 16499 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLR_strange | ( | ) | const |
Definition at line 16524 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLR_tau | ( | ) | const |
Definition at line 16504 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLR_up | ( | ) | const |
Definition at line 16509 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10892 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRL_bottom | ( | ) | const |
Definition at line 16564 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRL_charm | ( | ) | const |
Definition at line 16554 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRL_down | ( | ) | const |
Definition at line 16549 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRL_mu | ( | ) | const |
Definition at line 16534 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRL_strange | ( | ) | const |
Definition at line 16559 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRL_tau | ( | ) | const |
Definition at line 16539 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRL_up | ( | ) | const |
Definition at line 16544 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRR_bottom | ( | ) | const |
Definition at line 16600 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRR_charm | ( | ) | const |
Definition at line 16590 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRR_down | ( | ) | const |
Definition at line 16585 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRR_mu | ( | ) | const |
Definition at line 16569 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRR_strange | ( | ) | const |
Definition at line 16595 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRR_tau | ( | ) | const |
Definition at line 16574 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRR_up | ( | ) | const |
Definition at line 16580 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 15534 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 15558 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 15546 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 3042 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 3048 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 3031 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 3037 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 3053 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 3059 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 15524 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 3258 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 3296 of file NPSMEFTd6.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 3301 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 3279 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\).
Reimplemented from NPbase.
Definition at line 13819 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph].
Reimplemented from NPbase.
Definition at line 13862 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 3263 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 3381 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 3284 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\).
Reimplemented from NPbase.
Definition at line 3268 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\).
Reimplemented from NPbase.
Definition at line 3289 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltag3G | ( | ) | const |
The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\).
Definition at line 3541 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_Aff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 3534 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_Gff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 3520 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 3386 of file NPSMEFTd6.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 3391 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_hAff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 3513 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\).
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 3444 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_hGff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 3499 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\).
Reimplemented from NPbase.
Definition at line 3231 of file NPSMEFTd6.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 3236 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 3458 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_hZff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 3506 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_Zff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 3527 of file NPSMEFTd6.cpp.
|
virtual |
New physics contribution to the neutral-current axial-vector coupling \(g_A^f\).
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 3171 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\).
Reimplemented from NPbase.
Definition at line 3124 of file NPSMEFTd6.cpp.
The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\).
| [in] | fi | a lepton or quark |
| [in] | fj | a lepton or quark |
Reimplemented from NPbase.
Definition at line 3090 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHbbRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 12663 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHbbRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 12703 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHccRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 12598 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHccRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 12638 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHgagaRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 12417 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHgagaRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 12467 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHggRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.
Definition at line 10988 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHggRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11023 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHmumuRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 12493 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHmumuRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 12519 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHtautauRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 12545 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHtautauRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 12572 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWffRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11330 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWffRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11361 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWjjRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11214 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWjjRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11244 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWlvRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11097 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWlvRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11127 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWW2l2vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11153 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWW2l2vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11188 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWW4fRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11387 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWW4fRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11431 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWW4jRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11270 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWW4jRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11304 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWWRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11049 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWWRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11069 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZddRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 12124 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZddRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 12157 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZeeRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11564 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZeeRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11599 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZffRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 12183 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZffRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 12220 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZgaRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 12332 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZgaRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 12391 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZllRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11505 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZllRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11538 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZmumuRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11625 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZmumuRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11660 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZuuRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 12065 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZuuRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 12098 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZvvRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11944 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZvvRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11976 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ2e2muRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11819 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ2e2muRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11856 of file NPSMEFTd6.cpp.
|
inline |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 2523 of file NPSMEFTd6.h.
| double NPSMEFTd6::deltaGammaHZZ4dRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
| double NPSMEFTd6::deltaGammaHZZ4eRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11756 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4eRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11793 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4fRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 12246 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4fRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 12306 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4lRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11686 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4lRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11730 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4muRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11881 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4muRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11918 of file NPSMEFTd6.cpp.
|
inline |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 2506 of file NPSMEFTd6.h.
| double NPSMEFTd6::deltaGammaHZZ4uRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
| double NPSMEFTd6::deltaGammaHZZ4vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 12002 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 12039 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11457 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11477 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.
Definition at line 10909 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. Neglecting SM theory errors.
Definition at line 10931 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients.
Definition at line 10953 of file NPSMEFTd6.cpp.
|
virtual |
New physics contribution to the Fermi constant.
The new physics contribution \(\Delta G\) is defined as
\[ G_\mu = G_{\mu,\mathrm{SM}}(1+\Delta G)\,, \]
where \(G_\mu\) is the experimental value measured through muon decays, and \(G_{\mu,\mathrm{SM}}\) is the Fermi constant in the SM.
Reimplemented from NPbase.
Definition at line 2922 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGL_f | ( | const Particle | p | ) | const |
New physics contribution to the neutral-current left-handed coupling \(g_L^f\).
| [in] | f | a lepton or quark |
Definition at line 3176 of file NPSMEFTd6.cpp.
|
virtual |
New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 3207 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaGL_Wffh | ( | const Particle | pbar, |
| const Particle | p | ||
| ) | const |
The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Definition at line 3467 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGL_Zffh | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\).
| [in] | p | a lepton or quark |
Definition at line 3485 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 3020 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 3026 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGR_f | ( | const Particle | p | ) | const |
New physics contribution to the neutral-current right-handed coupling \(g_R^f\).
| [in] | f | a lepton or quark |
Definition at line 3191 of file NPSMEFTd6.cpp.
|
virtual |
New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 3222 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaGR_Wffh | ( | const Particle | pbar, |
| const Particle | p | ||
| ) | const |
The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Definition at line 3476 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGR_Zffh | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\).
| [in] | p | a lepton or quark |
Definition at line 3493 of file NPSMEFTd6.cpp.
|
virtual |
New physics contribution to the neutral-current vector coupling \(g_V^f\).
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 3166 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\).
Definition at line 3142 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\).
Definition at line 3147 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\).
Definition at line 3154 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\).
Definition at line 3159 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\).
Reimplemented from NPbase.
Definition at line 13836 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph].
Reimplemented from NPbase.
Definition at line 13875 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2987 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2993 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2998 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 3004 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2965 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2971 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2976 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2982 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 3009 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 3015 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\).
Definition at line 3075 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\).
Definition at line 3083 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2954 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2960 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 15480 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 15502 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 15513 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 15469 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 15491 of file NPSMEFTd6.cpp.
|
virtual |
The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle.
Reimplemented from NPbase.
Definition at line 13889 of file NPSMEFTd6.cpp.
|
virtual |
The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle.
< Gsl integral variable
< Gsl integral variable
< Gsl integral variable
Reimplemented from NPbase.
Definition at line 14188 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::f_triangle | ( | const double | tau | ) | const |
Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.
| [in] |
Definition at line 3551 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::g_triangle | ( | const double | tau | ) | const |
Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.
| [in] |
Definition at line 3563 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHbbRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model.
Definition at line 12648 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHccRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model.
Definition at line 12582 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHgagaRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model.
Definition at line 12401 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHggRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model.
Definition at line 10972 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHmumuRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model.
Definition at line 12477 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHtautauRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model.
Definition at line 12529 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHWffRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 11314 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHWjjRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model.
Definition at line 11198 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHWlvRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 11081 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHWW2l2vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 11137 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHWW4fRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 11371 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHWW4jRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model.
Definition at line 11254 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHWWRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model.
Definition at line 11033 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZddRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Zd d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.
Definition at line 12108 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZeeRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model.
Definition at line 11548 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZffRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 12167 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZgaRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model.
Definition at line 12316 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZllRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 11489 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZmumuRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model.
Definition at line 11609 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZuuRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Zu u)\) ( \(u=u,c \)) in the current model and in the Standard Model.
Definition at line 12049 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZvvRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model.
Definition at line 11928 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZZ2e2muRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model.
Definition at line 11803 of file NPSMEFTd6.cpp.
|
inline |
The ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.
Definition at line 2315 of file NPSMEFTd6.h.
| double NPSMEFTd6::GammaHZZ4eRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model.
Definition at line 11740 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZZ4fRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 12230 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZZ4lRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 11670 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZZ4muRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model.
Definition at line 11865 of file NPSMEFTd6.cpp.
|
inline |
The ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model.
Definition at line 2300 of file NPSMEFTd6.h.
| double NPSMEFTd6::GammaHZZ4vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model.
Definition at line 11986 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZZRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model.
Definition at line 11441 of file NPSMEFTd6.cpp.
|
virtual |
The total width of the \(W\) boson, \(\Gamma_W\).
Reimplemented from NPbase.
Definition at line 3137 of file NPSMEFTd6.cpp.
A partial decay width of the \(W\) boson decay into a SM fermion pair.
| [in] | fi | a lepton or quark |
| [in] | fj | a lepton or quark |
Reimplemented from NPbase.
Definition at line 3119 of file NPSMEFTd6.cpp.
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inlinevirtual |
A method to get the Matching object for this model.
Reimplemented from StandardModel.
Definition at line 961 of file NPSMEFTd6.h.
| gslpp::complex NPSMEFTd6::I_triangle_1 | ( | const double | tau, |
| const double | lambda | ||
| ) | const |
Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.
| [in] |
Definition at line 3575 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::I_triangle_2 | ( | const double | tau, |
| const double | lambda | ||
| ) | const |
Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.
| [in] |
Definition at line 3586 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\).
Reimplemented from NPbase.
Definition at line 15455 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\).
Reimplemented from NPbase.
Definition at line 15435 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\).
Reimplemented from NPbase.
Definition at line 15430 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\).
Reimplemented from NPbase.
Definition at line 15440 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\).
Reimplemented from NPbase.
Definition at line 15420 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\).
Reimplemented from NPbase.
Definition at line 15425 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\).
Reimplemented from NPbase.
Definition at line 15450 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\).
Reimplemented from NPbase.
Definition at line 15460 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\).
Reimplemented from NPbase.
Definition at line 15445 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\).
Reimplemented from NPbase.
Definition at line 13850 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 15608 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 4320 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 4655 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 9329 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 9526 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 4018 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 4311 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 14239 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 14396 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 5683 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 5997 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 7553 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 7910 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 7865 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 8894 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 7885 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 8914 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 6982 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 7073 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 3623 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13146 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12858 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].)
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 3679 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13074 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 9315 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13110 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13002 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13038 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12894 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12930 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12966 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 10182 of file NPSMEFTd6.cpp.
|
virtual |
The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class.
Reimplemented from NPbase.
Definition at line 14935 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{tHq}\) between the t-q-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 9220 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13692 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13188 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13566 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13629 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13440 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13503 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13251 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,Z\gamma\to \gamma 2\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\to \gamma 2\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13807 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13314 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13377 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ\to 4\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13798 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13746 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13242 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13620 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13683 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13494 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13557 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13305 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13368 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13431 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF}\) between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13755 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13701 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13197 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,inv}\) between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13760 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13575 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13638 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13449 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13512 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13260 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13323 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13386 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13728 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH}\) between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13769 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13224 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,inv}\) between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13781 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13602 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13665 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13476 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13539 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13287 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13350 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13413 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13719 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13215 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13593 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13656 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13467 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13530 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13278 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13341 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13404 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13710 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13206 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13584 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13647 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13458 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13521 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13269 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13332 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13395 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 9078 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13176 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12888 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13104 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13140 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13032 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13068 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12802 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12924 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12960 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12996 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 3758 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 3973 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13152 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12864 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13080 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13116 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13008 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13044 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12900 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12936 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12972 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 9063 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 9050 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13170 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12882 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13098 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13134 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13026 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13062 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12918 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12954 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12990 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 7188 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13164 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12876 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13092 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13128 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13020 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13056 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12912 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12948 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12984 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 7357 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13158 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12870 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13086 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13122 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13014 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 13050 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12906 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12942 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12978 of file NPSMEFTd6.cpp.
|
virtual |
The mass of the \(W\) boson, \(M_W\).
Reimplemented from NPbase.
Definition at line 3067 of file NPSMEFTd6.cpp.
|
virtual |
The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).)
Reimplemented from NPbase.
Definition at line 2927 of file NPSMEFTd6.cpp.
|
virtual |
The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).)
Reimplemented from NPbase.
Definition at line 2932 of file NPSMEFTd6.cpp.
|
virtual |
The oblique parameter \(U\).
Reimplemented from NPbase.
Definition at line 2937 of file NPSMEFTd6.cpp.
|
virtual |
The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).)
Reimplemented from NPbase.
Definition at line 2942 of file NPSMEFTd6.cpp.
|
virtual |
The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).)
Reimplemented from NPbase.
Definition at line 2947 of file NPSMEFTd6.cpp.
|
virtual |
The post-update method for NPSMEFTd6.
This method runs all the procedures that are need to be executed after the model is successfully updated.
Reimplemented from NPbase.
Definition at line 957 of file NPSMEFTd6.cpp.
|
virtual |
The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class.
Reimplemented from NPbase.
Definition at line 14899 of file NPSMEFTd6.cpp.
|
virtual |
A method to set a flag of NPSMEFTd6.
| [in] | name | name of a model flag |
| [in] | value | the boolean to be assigned to the flag specified by name |
Reimplemented from StandardModel.
Definition at line 2701 of file NPSMEFTd6.cpp.
|
protectedvirtual |
A method to set the value of a parameter of the model.
| [in] | name | name of a model parameter |
| [in] | value | the value to be assigned to the parameter specified by name |
Reimplemented from StandardModel.
Definition at line 1233 of file NPSMEFTd6.cpp.
|
virtual |
|
virtual |
|
virtual |
|
virtual |
|
virtual |
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15108 of file NPSMEFTd6.cpp.
|
virtual |
|
virtual |
|
virtual |
|
virtual |
|
virtual |
|
virtual |
|
virtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15256 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15268 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15276 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15288 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15300 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15216 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15208 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15226 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15236 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15246 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15198 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15188 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15168 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15159 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15153 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15178 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( ttH + tH \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15312 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15358 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15349 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15331 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15322 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15340 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15407 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15397 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15377 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15367 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 15387 of file NPSMEFTd6.cpp.
|
virtual |
Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\).
Reimplemented from NPbase.
Definition at line 14233 of file NPSMEFTd6.cpp.
|
protected |
Definition at line 5035 of file NPSMEFTd6.h.
|
protected |
Definition at line 5035 of file NPSMEFTd6.h.
|
protected |
Definition at line 5037 of file NPSMEFTd6.h.
|
protected |
Definition at line 5036 of file NPSMEFTd6.h.
|
protected |
Definition at line 5035 of file NPSMEFTd6.h.
|
protected |
Definition at line 5036 of file NPSMEFTd6.h.
|
protected |
Definition at line 5036 of file NPSMEFTd6.h.
|
protected |
Definition at line 5038 of file NPSMEFTd6.h.
|
protected |
Definition at line 5038 of file NPSMEFTd6.h.
|
protected |
Definition at line 5038 of file NPSMEFTd6.h.
|
protected |
Definition at line 5038 of file NPSMEFTd6.h.
|
protected |
Definition at line 5038 of file NPSMEFTd6.h.
|
protected |
Definition at line 5036 of file NPSMEFTd6.h.
|
protected |
Definition at line 5038 of file NPSMEFTd6.h.
|
protected |
Definition at line 5038 of file NPSMEFTd6.h.
|
protected |
Definition at line 5036 of file NPSMEFTd6.h.
|
protected |
Definition at line 5039 of file NPSMEFTd6.h.
|
protected |
Definition at line 5039 of file NPSMEFTd6.h.
|
protected |
Definition at line 5036 of file NPSMEFTd6.h.
|
protected |
The em constant at Mz.
Definition at line 4995 of file NPSMEFTd6.h.
|
protected |
The branching ratio of exotic (not invisible) Higgs decays.
Definition at line 4915 of file NPSMEFTd6.h.
|
protected |
The branching ratio of invisible Higgs decays.
Definition at line 4914 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{2W}\).
Definition at line 4475 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{2W}^{SILH}\).
Definition at line 4477 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{2B}\).
Definition at line 4476 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{2B}^{SILH}\).
Definition at line 4478 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{DB}\).
Definition at line 4486 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{11}\) (imaginary part).
Definition at line 4670 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{11}\) (real part).
Definition at line 4664 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{12}\) (imaginary part).
Definition at line 4671 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{12}\) (real part).
Definition at line 4665 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{13}\) (imaginary part).
Definition at line 4672 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{13}\) (real part).
Definition at line 4666 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{22}\) (imaginary part).
Definition at line 4673 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{22}\) (real part).
Definition at line 4667 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{23}\) (imaginary part).
Definition at line 4674 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{23}\) (real part).
Definition at line 4668 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{33}\) (imaginary part).
Definition at line 4675 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{33}\) (real part).
Definition at line 4669 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{11}\) (imaginary part).
Definition at line 4646 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{11}\) (real part).
Definition at line 4640 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{12}\) (imaginary part).
Definition at line 4647 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{12}\) (real part).
Definition at line 4641 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{13}\) (imaginary part).
Definition at line 4648 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{13}\) (real part).
Definition at line 4642 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{22}\) (imaginary part).
Definition at line 4649 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{22}\) (real part).
Definition at line 4643 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{23}\) (imaginary part).
Definition at line 4650 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{23}\) (real part).
Definition at line 4644 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{33}\) (imaginary part).
Definition at line 4651 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{33}\) (real part).
Definition at line 4645 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{11}\) (imaginary part).
Definition at line 4598 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{11}\) (real part).
Definition at line 4592 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{12}\) (imaginary part).
Definition at line 4599 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{12}\) (real part).
Definition at line 4593 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{13}\) (imaginary part).
Definition at line 4600 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{13}\) (real part).
Definition at line 4594 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{22}\) (imaginary part).
Definition at line 4601 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{22}\) (real part).
Definition at line 4595 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{23}\) (imaginary part).
Definition at line 4602 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{23}\) (real part).
Definition at line 4596 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{33}\) (imaginary part).
Definition at line 4603 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{33}\) (real part).
Definition at line 4597 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{DHB}\).
Definition at line 4484 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{DHW}\).
Definition at line 4485 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{DW}\).
Definition at line 4487 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{11}\) (imaginary part).
Definition at line 4658 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{11}\) (real part).
Definition at line 4652 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{12}\) (imaginary part).
Definition at line 4659 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{12}\) (real part).
Definition at line 4653 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{13}\) (imaginary part).
Definition at line 4660 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{13}\) (real part).
Definition at line 4654 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{22}\) (imaginary part).
Definition at line 4661 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{22}\) (real part).
Definition at line 4655 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{23}\) (imaginary part).
Definition at line 4662 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{23}\) (real part).
Definition at line 4656 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{33}\) (imaginary part).
Definition at line 4663 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{33}\) (real part).
Definition at line 4657 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{11}\) (imaginary part).
Definition at line 4694 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{11}\) (real part).
Definition at line 4688 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{12}\) (imaginary part).
Definition at line 4695 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{12}\) (real part).
Definition at line 4689 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{13}\) (imaginary part).
Definition at line 4696 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{13}\) (real part).
Definition at line 4690 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{22}\) (imaginary part).
Definition at line 4697 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{22}\) (real part).
Definition at line 4691 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{23}\) (imaginary part).
Definition at line 4698 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{23}\) (real part).
Definition at line 4692 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{33}\) (imaginary part).
Definition at line 4699 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{33}\) (real part).
Definition at line 4693 of file NPSMEFTd6.h.
|
protected |
Definition at line 4720 of file NPSMEFTd6.h.
|
protected |
Definition at line 4721 of file NPSMEFTd6.h.
|
protected |
Definition at line 4723 of file NPSMEFTd6.h.
|
protected |
Definition at line 4724 of file NPSMEFTd6.h.
|
protected |
Definition at line 4722 of file NPSMEFTd6.h.
|
protected |
Definition at line 4721 of file NPSMEFTd6.h.
|
protected |
Definition at line 4723 of file NPSMEFTd6.h.
|
protected |
Definition at line 4724 of file NPSMEFTd6.h.
|
protected |
Definition at line 4722 of file NPSMEFTd6.h.
|
protected |
Definition at line 4723 of file NPSMEFTd6.h.
|
protected |
Definition at line 4724 of file NPSMEFTd6.h.
|
protected |
Definition at line 4713 of file NPSMEFTd6.h.
|
protected |
Definition at line 4714 of file NPSMEFTd6.h.
|
protected |
Definition at line 4715 of file NPSMEFTd6.h.
|
protected |
Definition at line 4714 of file NPSMEFTd6.h.
|
protected |
Definition at line 4715 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{11}\) (imaginary part).
Definition at line 4574 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{11}\) (real part).
Definition at line 4568 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{12}\) (imaginary part).
Definition at line 4575 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{12}\) (real part).
Definition at line 4569 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{13}\) (imaginary part).
Definition at line 4576 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{13}\) (real part).
Definition at line 4570 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{22}\) (imaginary part).
Definition at line 4577 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{22}\) (real part).
Definition at line 4571 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{23}\) (imaginary part).
Definition at line 4578 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{23}\) (real part).
Definition at line 4572 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{33}\) (imaginary part).
Definition at line 4579 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{33}\) (real part).
Definition at line 4573 of file NPSMEFTd6.h.
|
protected |
Definition at line 4716 of file NPSMEFTd6.h.
|
protected |
Definition at line 4717 of file NPSMEFTd6.h.
|
protected |
Definition at line 4718 of file NPSMEFTd6.h.
|
protected |
Definition at line 4717 of file NPSMEFTd6.h.
|
protected |
Definition at line 4719 of file NPSMEFTd6.h.
|
protected |
Definition at line 4718 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{11}\) (imaginary part).
Definition at line 4682 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{11}\) (real part).
Definition at line 4676 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{12}\) (imaginary part).
Definition at line 4683 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{12}\) (real part).
Definition at line 4677 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{13}\) (imaginary part).
Definition at line 4684 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{13}\) (real part).
Definition at line 4678 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{22}\) (imaginary part).
Definition at line 4685 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{22}\) (real part).
Definition at line 4679 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{23}\) (imaginary part).
Definition at line 4686 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{23}\) (real part).
Definition at line 4680 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{33}\) (imaginary part).
Definition at line 4687 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{33}\) (real part).
Definition at line 4681 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{G}\).
Definition at line 4473 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{H}\).
Definition at line 4492 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{HB}\).
Definition at line 4481 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{H\Box}\).
Definition at line 4491 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{HD}\).
Definition at line 4489 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{11}\).
Definition at line 4547 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{12}\) (imaginary part).
Definition at line 4553 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{12}\) (real part).
Definition at line 4548 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{13}\) (imaginary part).
Definition at line 4554 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{13}\) (real part).
Definition at line 4549 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{22}\).
Definition at line 4550 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{23}\) (imaginary part).
Definition at line 4555 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{23}\) (real part).
Definition at line 4551 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{33}\).
Definition at line 4552 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{11}\).
Definition at line 4511 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{12}\) (imaginary part).
Definition at line 4517 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{12}\) (real part).
Definition at line 4512 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{13}\) (imaginary part).
Definition at line 4518 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{13}\) (real part).
Definition at line 4513 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{22}\).
Definition at line 4514 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{23}\) (imaginary part).
Definition at line 4519 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{23}\) (real part).
Definition at line 4515 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{33}\).
Definition at line 4516 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{HG}\).
Definition at line 4479 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\).
Definition at line 4493 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part).
Definition at line 4499 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part).
Definition at line 4494 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part).
Definition at line 4500 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part).
Definition at line 4495 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\).
Definition at line 4496 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part).
Definition at line 4501 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part).
Definition at line 4497 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\).
Definition at line 4498 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\).
Definition at line 4502 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).
Definition at line 4508 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).
Definition at line 4503 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).
Definition at line 4509 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).
Definition at line 4504 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\).
Definition at line 4505 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).
Definition at line 4510 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).
Definition at line 4506 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\).
Definition at line 4507 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\).
Definition at line 4520 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part).
Definition at line 4526 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part).
Definition at line 4521 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part).
Definition at line 4527 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part).
Definition at line 4522 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\).
Definition at line 4523 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part).
Definition at line 4528 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part).
Definition at line 4524 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\).
Definition at line 4525 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\).
Definition at line 4529 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part).
Definition at line 4535 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part).
Definition at line 4530 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part).
Definition at line 4536 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part).
Definition at line 4531 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\).
Definition at line 4532 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part).
Definition at line 4537 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part).
Definition at line 4533 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\).
Definition at line 4534 of file NPSMEFTd6.h.
|
protected |
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes.
Definition at line 5024 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{11}\).
Definition at line 4538 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{12}\) (imaginary part).
Definition at line 4544 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{12}\) (real part).
Definition at line 4539 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{13}\) (imaginary part).
Definition at line 4545 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{13}\) (real part).
Definition at line 4540 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{22}\).
Definition at line 4541 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{23}\) (imaginary part).
Definition at line 4546 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{23}\) (real part).
Definition at line 4542 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{33}\).
Definition at line 4543 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{11}\) (imaginary part).
Definition at line 4562 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{11}\) (real part).
Definition at line 4556 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{12}\) (imaginary part).
Definition at line 4563 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{12}\) (real part).
Definition at line 4557 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{13}\) (imaginary part).
Definition at line 4564 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{13}\) (real part).
Definition at line 4558 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{22}\) (imaginary part).
Definition at line 4565 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{22}\) (real part).
Definition at line 4559 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{23}\) (imaginary part).
Definition at line 4566 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{23}\) (real part).
Definition at line 4560 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{33}\) (imaginary part).
Definition at line 4567 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{33}\) (real part).
Definition at line 4561 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{HW}\).
Definition at line 4480 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{HWB}\).
Definition at line 4488 of file NPSMEFTd6.h.
|
protected |
The combination of dimension-6 operator coefficients entering in \(\delta_{AA}\): \(s_W^2 C_{HW} + c_W^2 C_{HW}\).
Definition at line 4482 of file NPSMEFTd6.h.
|
protected |
The combination of dimension-6 operator coefficients \(-c_W^2 C_{HW} + s_W^2 C_{HW}\).
Definition at line 4483 of file NPSMEFTd6.h.
|
protected |
Definition at line 4974 of file NPSMEFTd6.h.
|
protected |
Definition at line 4975 of file NPSMEFTd6.h.
|
protected |
Definition at line 4976 of file NPSMEFTd6.h.
|
protected |
Definition at line 4958 of file NPSMEFTd6.h.
|
protected |
Definition at line 4959 of file NPSMEFTd6.h.
|
protected |
Definition at line 4966 of file NPSMEFTd6.h.
|
protected |
Definition at line 4967 of file NPSMEFTd6.h.
|
protected |
Definition at line 4968 of file NPSMEFTd6.h.
|
protected |
Definition at line 4964 of file NPSMEFTd6.h.
|
protected |
Definition at line 4957 of file NPSMEFTd6.h.
|
protected |
Definition at line 4962 of file NPSMEFTd6.h.
|
protected |
Definition at line 4963 of file NPSMEFTd6.h.
|
protected |
Definition at line 4950 of file NPSMEFTd6.h.
|
protected |
Definition at line 4951 of file NPSMEFTd6.h.
|
protected |
Definition at line 4952 of file NPSMEFTd6.h.
|
protected |
Definition at line 4942 of file NPSMEFTd6.h.
|
protected |
Definition at line 4943 of file NPSMEFTd6.h.
|
protected |
Definition at line 4944 of file NPSMEFTd6.h.
|
protected |
Definition at line 4928 of file NPSMEFTd6.h.
|
protected |
Definition at line 4929 of file NPSMEFTd6.h.
|
protected |
Definition at line 4930 of file NPSMEFTd6.h.
|
protected |
Definition at line 4931 of file NPSMEFTd6.h.
|
protected |
Definition at line 4932 of file NPSMEFTd6.h.
|
protected |
Definition at line 4933 of file NPSMEFTd6.h.
|
protected |
Definition at line 4935 of file NPSMEFTd6.h.
|
protected |
Definition at line 4936 of file NPSMEFTd6.h.
|
protected |
Definition at line 4937 of file NPSMEFTd6.h.
|
protected |
Definition at line 4938 of file NPSMEFTd6.h.
|
protected |
Definition at line 4939 of file NPSMEFTd6.h.
|
protected |
Definition at line 4940 of file NPSMEFTd6.h.
|
protected |
Definition at line 4946 of file NPSMEFTd6.h.
|
protected |
Definition at line 4947 of file NPSMEFTd6.h.
|
protected |
Definition at line 4948 of file NPSMEFTd6.h.
|
protected |
Definition at line 4956 of file NPSMEFTd6.h.
|
protected |
Definition at line 4960 of file NPSMEFTd6.h.
|
protected |
Definition at line 4990 of file NPSMEFTd6.h.
|
protected |
Definition at line 4991 of file NPSMEFTd6.h.
|
protected |
Definition at line 4986 of file NPSMEFTd6.h.
|
protected |
Definition at line 4987 of file NPSMEFTd6.h.
|
protected |
Definition at line 4988 of file NPSMEFTd6.h.
|
protected |
Definition at line 4978 of file NPSMEFTd6.h.
|
protected |
Definition at line 4979 of file NPSMEFTd6.h.
|
protected |
Definition at line 4980 of file NPSMEFTd6.h.
|
protected |
Definition at line 4970 of file NPSMEFTd6.h.
|
protected |
Definition at line 4971 of file NPSMEFTd6.h.
|
protected |
Definition at line 4972 of file NPSMEFTd6.h.
|
protected |
Definition at line 4982 of file NPSMEFTd6.h.
|
protected |
Definition at line 4983 of file NPSMEFTd6.h.
|
protected |
Definition at line 4984 of file NPSMEFTd6.h.
|
protected |
Definition at line 4954 of file NPSMEFTd6.h.
|
protected |
Definition at line 4732 of file NPSMEFTd6.h.
|
protected |
Definition at line 4733 of file NPSMEFTd6.h.
|
protected |
Definition at line 4735 of file NPSMEFTd6.h.
|
protected |
Definition at line 4736 of file NPSMEFTd6.h.
|
protected |
Definition at line 4734 of file NPSMEFTd6.h.
|
protected |
Definition at line 4733 of file NPSMEFTd6.h.
|
protected |
Definition at line 4735 of file NPSMEFTd6.h.
|
protected |
Definition at line 4736 of file NPSMEFTd6.h.
|
protected |
Definition at line 4734 of file NPSMEFTd6.h.
|
protected |
Definition at line 4735 of file NPSMEFTd6.h.
|
protected |
Definition at line 4736 of file NPSMEFTd6.h.
|
protected |
Definition at line 4725 of file NPSMEFTd6.h.
|
protected |
Definition at line 4726 of file NPSMEFTd6.h.
|
protected |
Definition at line 4727 of file NPSMEFTd6.h.
|
protected |
Definition at line 4726 of file NPSMEFTd6.h.
|
protected |
Definition at line 4727 of file NPSMEFTd6.h.
|
protected |
Definition at line 4742 of file NPSMEFTd6.h.
|
protected |
Definition at line 4742 of file NPSMEFTd6.h.
|
protected |
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions modifying the Higgs trilinear coupling (Quadratic terms).
Definition at line 5028 of file NPSMEFTd6.h.
|
protected |
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions.
Definition at line 5026 of file NPSMEFTd6.h.
|
protected |
Definition at line 4700 of file NPSMEFTd6.h.
|
protected |
Definition at line 4701 of file NPSMEFTd6.h.
|
protected |
Definition at line 4702 of file NPSMEFTd6.h.
|
protected |
Definition at line 4701 of file NPSMEFTd6.h.
|
protected |
Definition at line 4702 of file NPSMEFTd6.h.
|
protected |
Definition at line 4701 of file NPSMEFTd6.h.
|
protected |
Definition at line 4701 of file NPSMEFTd6.h.
|
protected |
Definition at line 4702 of file NPSMEFTd6.h.
|
protected |
Definition at line 4702 of file NPSMEFTd6.h.
|
protected |
Definition at line 4703 of file NPSMEFTd6.h.
|
protected |
Definition at line 4704 of file NPSMEFTd6.h.
|
protected |
Definition at line 4706 of file NPSMEFTd6.h.
|
protected |
Definition at line 4707 of file NPSMEFTd6.h.
|
protected |
Definition at line 4705 of file NPSMEFTd6.h.
|
protected |
Definition at line 4704 of file NPSMEFTd6.h.
|
protected |
Definition at line 4705 of file NPSMEFTd6.h.
|
protected |
Definition at line 4704 of file NPSMEFTd6.h.
|
protected |
Definition at line 4704 of file NPSMEFTd6.h.
|
protected |
Definition at line 4706 of file NPSMEFTd6.h.
|
protected |
Definition at line 4707 of file NPSMEFTd6.h.
|
protected |
Definition at line 4705 of file NPSMEFTd6.h.
|
protected |
Definition at line 4705 of file NPSMEFTd6.h.
|
protected |
Definition at line 4706 of file NPSMEFTd6.h.
|
protected |
Definition at line 4707 of file NPSMEFTd6.h.
|
protected |
Definition at line 4708 of file NPSMEFTd6.h.
|
protected |
Definition at line 4709 of file NPSMEFTd6.h.
|
protected |
Definition at line 4711 of file NPSMEFTd6.h.
|
protected |
Definition at line 4712 of file NPSMEFTd6.h.
|
protected |
Definition at line 4710 of file NPSMEFTd6.h.
|
protected |
Definition at line 4709 of file NPSMEFTd6.h.
|
protected |
Definition at line 4710 of file NPSMEFTd6.h.
|
protected |
Definition at line 4709 of file NPSMEFTd6.h.
|
protected |
Definition at line 4709 of file NPSMEFTd6.h.
|
protected |
Definition at line 4711 of file NPSMEFTd6.h.
|
protected |
Definition at line 4712 of file NPSMEFTd6.h.
|
protected |
Definition at line 4710 of file NPSMEFTd6.h.
|
protected |
Definition at line 4710 of file NPSMEFTd6.h.
|
protected |
Definition at line 4711 of file NPSMEFTd6.h.
|
protected |
Definition at line 4712 of file NPSMEFTd6.h.
|
protected |
Definition at line 4728 of file NPSMEFTd6.h.
|
protected |
Definition at line 4729 of file NPSMEFTd6.h.
|
protected |
Definition at line 4730 of file NPSMEFTd6.h.
|
protected |
Definition at line 4729 of file NPSMEFTd6.h.
|
protected |
Definition at line 4731 of file NPSMEFTd6.h.
|
protected |
Definition at line 4730 of file NPSMEFTd6.h.
|
protected |
Definition at line 4742 of file NPSMEFTd6.h.
|
protected |
Definition at line 4742 of file NPSMEFTd6.h.
|
protected |
Definition at line 4737 of file NPSMEFTd6.h.
|
protected |
Definition at line 4738 of file NPSMEFTd6.h.
|
protected |
Definition at line 4739 of file NPSMEFTd6.h.
|
protected |
Definition at line 4738 of file NPSMEFTd6.h.
|
protected |
Definition at line 4740 of file NPSMEFTd6.h.
|
protected |
Definition at line 4740 of file NPSMEFTd6.h.
|
protected |
Definition at line 4740 of file NPSMEFTd6.h.
|
protected |
Definition at line 4741 of file NPSMEFTd6.h.
|
protected |
Definition at line 4741 of file NPSMEFTd6.h.
|
protected |
Definition at line 4741 of file NPSMEFTd6.h.
|
protected |
Definition at line 4739 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{T}\).
Definition at line 4490 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{11}\) (imaginary part).
Definition at line 4634 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{11}\) (real part).
Definition at line 4628 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{12}\) (imaginary part).
Definition at line 4635 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{12}\) (real part).
Definition at line 4629 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{13}\) (imaginary part).
Definition at line 4636 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{13}\) (real part).
Definition at line 4630 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{22}\) (imaginary part).
Definition at line 4637 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{22}\) (real part).
Definition at line 4631 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{23}\) (imaginary part).
Definition at line 4638 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{23}\) (real part).
Definition at line 4632 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{33}\) (imaginary part).
Definition at line 4639 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{33}\) (real part).
Definition at line 4633 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{11}\) (imaginary part).
Definition at line 4610 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{11}\) (real part).
Definition at line 4604 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{12}\) (imaginary part).
Definition at line 4611 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{12}\) (real part).
Definition at line 4605 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{13}\) (imaginary part).
Definition at line 4612 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{13}\) (real part).
Definition at line 4606 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{22}\) (imaginary part).
Definition at line 4613 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{22}\) (real part).
Definition at line 4607 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{23}\) (imaginary part).
Definition at line 4614 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{23}\) (real part).
Definition at line 4608 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{33}\) (imaginary part).
Definition at line 4615 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{33}\) (real part).
Definition at line 4609 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{11}\) (imaginary part).
Definition at line 4586 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{11}\) (real part).
Definition at line 4580 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{12}\) (imaginary part).
Definition at line 4587 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{12}\) (real part).
Definition at line 4581 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{13}\) (imaginary part).
Definition at line 4588 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{13}\) (real part).
Definition at line 4582 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{22}\) (imaginary part).
Definition at line 4589 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{22}\) (real part).
Definition at line 4583 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{23}\) (imaginary part).
Definition at line 4590 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{23}\) (real part).
Definition at line 4584 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{33}\) (imaginary part).
Definition at line 4591 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{33}\) (real part).
Definition at line 4585 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{11}\) (imaginary part).
Definition at line 4622 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{11}\) (real part).
Definition at line 4616 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{12}\) (imaginary part).
Definition at line 4623 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{12}\) (real part).
Definition at line 4617 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{13}\) (imaginary part).
Definition at line 4624 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{13}\) (real part).
Definition at line 4618 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{22}\) (imaginary part).
Definition at line 4625 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{22}\) (real part).
Definition at line 4619 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{23}\) (imaginary part).
Definition at line 4626 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{23}\) (real part).
Definition at line 4620 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{33}\) (imaginary part).
Definition at line 4627 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{33}\) (real part).
Definition at line 4621 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{W}\).
Definition at line 4474 of file NPSMEFTd6.h.
|
protected |
The square of the tree level values for the cosine of the weak angle.
Definition at line 5000 of file NPSMEFTd6.h.
|
protected |
The tree level values for the cosine of the weak angle.
Definition at line 4998 of file NPSMEFTd6.h.
|
protected |
Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.
Definition at line 5016 of file NPSMEFTd6.h.
|
protected |
Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.
Definition at line 5017 of file NPSMEFTd6.h.
|
protected |
Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition.
Definition at line 5018 of file NPSMEFTd6.h.
|
protected |
Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition.
Definition at line 5015 of file NPSMEFTd6.h.
|
protected |
Independent contribution to aTGC.
Definition at line 4917 of file NPSMEFTd6.h.
|
protected |
Definition at line 5042 of file NPSMEFTd6.h.
|
protected |
Definition at line 5042 of file NPSMEFTd6.h.
|
protected |
Independent contribution to aTGC.
Definition at line 4918 of file NPSMEFTd6.h.
|
protected |
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition at line 5022 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.)
Definition at line 4759 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.)
Definition at line 4760 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.)
Definition at line 4755 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.)
Definition at line 4756 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.)
Definition at line 4757 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.)
Definition at line 4758 of file NPSMEFTd6.h.
|
protected |
The em coupling at Mz.
Definition at line 4996 of file NPSMEFTd6.h.
|
protected |
The em coupling squared (at Mz).
Definition at line 4997 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.)
Definition at line 4761 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.)
Definition at line 4762 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.)
Definition at line 4763 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.)
Definition at line 4764 of file NPSMEFTd6.h.
|
protected |
Definition at line 4784 of file NPSMEFTd6.h.
|
protected |
Definition at line 4784 of file NPSMEFTd6.h.
|
protected |
Total relative theoretical error in \(gg \to H \to X\).
Definition at line 4784 of file NPSMEFTd6.h.
|
protected |
Definition at line 4784 of file NPSMEFTd6.h.
|
protected |
Definition at line 4784 of file NPSMEFTd6.h.
|
protected |
Definition at line 4784 of file NPSMEFTd6.h.
|
protected |
Definition at line 4784 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.)
Definition at line 4745 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.)
Definition at line 4746 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to b\bar{b}\).
Definition at line 4781 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to b\bar{b}\).
Definition at line 4782 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to c\bar{c}\).
Definition at line 4779 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to c\bar{c}\).
Definition at line 4780 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to \gamma\gamma\).
Definition at line 4773 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to \gamma\gamma\).
Definition at line 4774 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to g g\).
Definition at line 4765 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to g g\).
Definition at line 4766 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to \mu^+ \mu^-\).
Definition at line 4775 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to \mu^+ \mu^-\).
Definition at line 4776 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to \tau^+ \tau^-\).
Definition at line 4777 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to \tau^+ \tau^-\).
Definition at line 4778 of file NPSMEFTd6.h.
|
protected |
Total relative theoretical error in the Higgs width.
Definition at line 4791 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to W W\).
Definition at line 4767 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to W W\).
Definition at line 4768 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to Z \gamma\).
Definition at line 4771 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to Z \gamma\).
Definition at line 4772 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to Z Z\).
Definition at line 4769 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to Z Z\).
Definition at line 4770 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (13 & 14 TeV).
Definition at line 4912 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (13 & 14 TeV).
Definition at line 4910 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (13 & 14 TeV).
Definition at line 4909 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (13 & 14 TeV).
Definition at line 4911 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (1.96 TeV).
Definition at line 4902 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (1.96 TeV).
Definition at line 4900 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (1.96 TeV).
Definition at line 4899 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (1.96 TeV).
Definition at line 4901 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (7 & 8 TeV).
Definition at line 4907 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (7 & 8 TeV).
Definition at line 4905 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (7 & 8 TeV).
Definition at line 4904 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (7 & 8 TeV).
Definition at line 4906 of file NPSMEFTd6.h.
|
protected |
Definition at line 4788 of file NPSMEFTd6.h.
|
protected |
Definition at line 4788 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.)
Definition at line 4747 of file NPSMEFTd6.h.
|
protected |
Total relative theoretical error in \(pp \to ttH \to tt X\).
Definition at line 4788 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.)
Definition at line 4748 of file NPSMEFTd6.h.
|
protected |
Definition at line 4788 of file NPSMEFTd6.h.
|
protected |
Definition at line 4788 of file NPSMEFTd6.h.
|
protected |
Definition at line 4788 of file NPSMEFTd6.h.
|
protected |
Definition at line 4788 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 4834 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 4832 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 4833 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 4828 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 4822 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 4827 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 4825 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 4831 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 4823 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 4826 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 4824 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 4829 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 4830 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 4806 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 4804 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 4805 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 4800 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 4794 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 4799 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 4797 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 4803 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 4795 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 4798 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 4796 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 4801 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 4802 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 4820 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 4818 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 4819 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 4814 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 4808 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 4813 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 4811 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 4817 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 4809 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 4812 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 4810 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 4815 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 4816 of file NPSMEFTd6.h.
|
protected |
Definition at line 4785 of file NPSMEFTd6.h.
|
protected |
Definition at line 4785 of file NPSMEFTd6.h.
|
protected |
Definition at line 4789 of file NPSMEFTd6.h.
|
protected |
Total relative theoretical error in \(pp \to Hjj (VBF) \to X jj\).
Definition at line 4785 of file NPSMEFTd6.h.
|
protected |
Definition at line 4785 of file NPSMEFTd6.h.
|
protected |
Definition at line 4785 of file NPSMEFTd6.h.
|
protected |
Definition at line 4785 of file NPSMEFTd6.h.
|
protected |
Definition at line 4785 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.)
Definition at line 4749 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.)
Definition at line 4750 of file NPSMEFTd6.h.
|
protected |
Total relative theoretical error in \(pp \to X H \to X + invisible\).
Definition at line 4789 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (13 & 14 TeV).
Definition at line 4858 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (13 & 14 TeV).
Definition at line 4857 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (13 & 14 TeV).
Definition at line 4852 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (13 & 14 TeV).
Definition at line 4854 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (13 & 14 TeV).
Definition at line 4853 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (13 & 14 TeV).
Definition at line 4855 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (13 & 14 TeV).
Definition at line 4856 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (1.96 TeV).
Definition at line 4842 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (1.96 TeV).
Definition at line 4841 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (1.96 TeV).
Definition at line 4836 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (1.96 TeV).
Definition at line 4838 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (1.96 TeV).
Definition at line 4837 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (1.96 TeV).
Definition at line 4839 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (1.96 TeV).
Definition at line 4840 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (7 & 8 TeV).
Definition at line 4850 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (7 & 8 TeV).
Definition at line 4849 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (7 & 8 TeV).
Definition at line 4844 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (7 & 8 TeV).
Definition at line 4846 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (7 & 8 TeV).
Definition at line 4845 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (7 & 8 TeV).
Definition at line 4847 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (7 & 8 TeV).
Definition at line 4848 of file NPSMEFTd6.h.
|
protected |
Definition at line 4786 of file NPSMEFTd6.h.
|
protected |
Definition at line 4786 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.)
Definition at line 4751 of file NPSMEFTd6.h.
|
protected |
Total relative theoretical error in \(pp \to WH \to W X\).
Definition at line 4786 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in WH production. (Assumed to be constant in energy.)
Definition at line 4752 of file NPSMEFTd6.h.
|
protected |
Definition at line 4786 of file NPSMEFTd6.h.
|
protected |
Definition at line 4786 of file NPSMEFTd6.h.
|
protected |
Definition at line 4786 of file NPSMEFTd6.h.
|
protected |
Definition at line 4786 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 4897 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 4895 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 4896 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 4892 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 4886 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 4891 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 4889 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 4887 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 4890 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 4888 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 4893 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 4894 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 4871 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 4869 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 4870 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 4866 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 4860 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 4865 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 4863 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 4861 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 4864 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 4862 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 4867 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 4868 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 4884 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 4882 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 4883 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 4879 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 4873 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 4878 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 4876 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 4874 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 4877 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 4875 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 4880 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 4881 of file NPSMEFTd6.h.
|
protected |
Definition at line 4787 of file NPSMEFTd6.h.
|
protected |
Definition at line 4787 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.)
Definition at line 4753 of file NPSMEFTd6.h.
|
protected |
Total relative theoretical error in \(pp \to ZH \to Z X\).
Definition at line 4787 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.)
Definition at line 4754 of file NPSMEFTd6.h.
|
protected |
Definition at line 4787 of file NPSMEFTd6.h.
|
protected |
Definition at line 4787 of file NPSMEFTd6.h.
|
protected |
Definition at line 4787 of file NPSMEFTd6.h.
|
protected |
Definition at line 4787 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients.
Definition at line 5107 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables.
Definition at line 5109 of file NPSMEFTd6.h.
|
private |
An internal boolean flag that is true if assuming lepton flavour universality.
Definition at line 5117 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling.
Definition at line 5111 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if including modifications in the SM loops in Higgs observables due to the dim 6 interactions.
Definition at line 5110 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd family in the CHF operators.
Definition at line 5106 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on.
Definition at line 5104 of file NPSMEFTd6.h.
|
private |
An internal boolean flag that is true if assuming quark flavour universality.
Definition at line 5123 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and CHB.
Definition at line 5105 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and all proportional to the same coefficient (CuH_33 and CuV_33 respectively).
Definition at line 5108 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(U(1)_Y\) gauge coupling contant (at the \(Z\) pole).
Definition at line 5003 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(SU(2)_L\) gauge coupling contant (at the \(Z\) pole).
Definition at line 5004 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(SU(3)_c\) gauge coupling contant (at the \(Z\) pole).
Definition at line 5005 of file NPSMEFTd6.h.
|
protected |
NP contributions and Total to Higgs width ratio with SM.
Definition at line 5042 of file NPSMEFTd6.h.
|
protected |
Definition at line 5010 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(Z\bar{d}d\) couplings in the SM.
Definition at line 5010 of file NPSMEFTd6.h.
|
protected |
Definition at line 5008 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(Z\ell^+\ell^-\) couplings in the SM.
Definition at line 5008 of file NPSMEFTd6.h.
|
protected |
Definition at line 5009 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(Z\bar{u}u\) couplings in the SM.
Definition at line 5009 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(Z\bar{\nu}\nu\) couplings in the SM.
Definition at line 5007 of file NPSMEFTd6.h.
|
protected |
The new physics scale [GeV].
Definition at line 4743 of file NPSMEFTd6.h.
|
protected |
The SM tree level value of the scalar quartic coupling in the potential.
Definition at line 5020 of file NPSMEFTd6.h.
|
protected |
The square of the new physics scale [GeV \(^2\)].
Definition at line 4925 of file NPSMEFTd6.h.
|
protected |
Independent contribution to aTGC.
Definition at line 4919 of file NPSMEFTd6.h.
|
static |
|
static |
The number of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities.
　
Definition at line 909 of file NPSMEFTd6.h.
|
mutableprotected |
Definition at line 4471 of file NPSMEFTd6.h.
|
static |
A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=false.
Definition at line 897 of file NPSMEFTd6.h.
|
static |
A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=false.
Definition at line 916 of file NPSMEFTd6.h.
|
static |
A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=true.
Definition at line 903 of file NPSMEFTd6.h.
|
static |
A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=true.
Definition at line 923 of file NPSMEFTd6.h.
|
protected |
The square of the tree level values for the sine of the weak angle.
Definition at line 5001 of file NPSMEFTd6.h.
|
protected |
The tree level values for the sine of the weak angle.
Definition at line 4999 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(W^-\bar{\ell}\nu\) couplings in the SM. (Neglecting PMNS effects.)
Definition at line 5012 of file NPSMEFTd6.h.
|
protected |
The square of the EW vev.
Definition at line 4993 of file NPSMEFTd6.h.
|
protected |
The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\).
Definition at line 4994 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(W^+\bar{u}d\) couplings in the SM. (Neglecting CKM effects.)
Definition at line 5013 of file NPSMEFTd6.h.
|
private |
Gsl integral variable
Definition at line 5125 of file NPSMEFTd6.h.
|
protected |
SM d-quark Yukawas.
Definition at line 5032 of file NPSMEFTd6.h.
|
protected |
Definition at line 5031 of file NPSMEFTd6.h.
|
protected |
Definition at line 5032 of file NPSMEFTd6.h.
|
protected |
Definition at line 5030 of file NPSMEFTd6.h.
|
protected |
Definition at line 5030 of file NPSMEFTd6.h.
|
protected |
Definition at line 5032 of file NPSMEFTd6.h.
|
protected |
SM u-quark Yukawas.
Definition at line 5031 of file NPSMEFTd6.h.
|
protected |
SM lepton Yukawas.
Definition at line 5030 of file NPSMEFTd6.h.
|
protected |
Definition at line 5031 of file NPSMEFTd6.h.
1.8.16 